PART III.

TROPISM IN PLANTS.

XXII.--THE BALANCED CRESCOGRAPH

_By_

SIR J. C. BOSE.

We shall in the succeeding series of papers deal with the subject of

tropism in general. Different plant organs undergo curvature or bending,

sometimes towards and at other times away from the stimulus which

induces it. The problem is very intricate; the possibility of its

solution will depend greatly on the accurate determination of the

immediate and after-effects of various stimuli on the responding organ.

The curvature induced in the growing organ is brought about by

variation, often extremely slight, of the rate of growth; the result,

moreover, is liable to be modified by the duration and point of

application of stimulus. The difficulties connected with the problem can

only be removed by the detection and measurement of the minutest

variation in growth, and by securing a continuous and automatic record

of the entire history of the change.

In the chapter on High Magnification Crescograph an account is given of

the apparatus which I have devised by which the rate of growth may be

magnified from ten thousand to ten millions times. It is thus possible

to measure the imperceptible growth of plants for a period shorter than

a single second. The variation of normal rate of growth is also found by

measuring successive growth records on a stationary plate at regular

intervals, say of ten seconds, or from the flexure in the growth-curve

taken on a moving plate (p. 163).

I was next desirous of exalting the sensitiveness to a still higher

degree by an independent method, which would not only reveal very

slight variation induced in the rate of growth, but also the latent

period and time-relations of the change. For this purpose I at first

devised the Optical Method of Balance[1] which was considered at the

time to be extremely sensitive. The spot of light from the Optical Lever

(which magnified the rate of growth) was made to fall upon a mirror to

which a compensating movement was imparted so that the light-spot after

double reflection remained stationary. Any change of rate of

growth--acceleration or retardation--was at once detected by the

movement of the hitherto stationary spot of light in one direction or

the other.

[1] "Plant Response"--p. 413.

A very careful manipulation was required for the adjustment of the

Optical Balance; the record moreover was not automatic. For these

reasons I have been engaged for several years past in perfecting a new

apparatus by which, (1) the balance could be directly obtained with the

utmost exactitude, (2) where an attached scale would indicate the exact

rate of growth, and (3) in which the upsetting of the balance by

external stimulus would be automatically recorded, the curve giving the

time relations of the change.

PRINCIPLE OF THE METHOD OF BALANCE.

I shall take a concrete example in explanation of the method of balance.

Taking the rate of growth per second of a plant to be 1/50,000 inch or

0·5 µ, per second (equal to the wave length of sodium light), the tip of

the plant will be maintained at the same point in space if we succeeded

in making the plant-holder subside exactly at the same rate. The

growth-elongation of the plant will then be exactly balanced by a

compensating movement downwards. The state of exact balance is indicated

when the recording lever of the Crescograph traces a horizontal line on

the moving plate. Overbalance or underbalance will deflect the record

below or above the horizontal line.

[Illustration: FIG. 93.--Arrangement for compensation of growth-movement

by equal subsidence of plant-holder; S, adjusting screw for regulation

of speed of rotation; G, governor; W, heavy weight; P, plant-holder.]

COMPENSATING MOVEMENT.

For securing exact balance the holder of the plant P, in the given

example, will have to subside at a rate of 1/50,000 inch per second.

This is accomplished by a system of reducing worm and pinion, also of

clock wheels (Fig. 93). The clock at first used for this purpose was

worked by the usual balance wheel. Though this secured an _average_

balance yet as each tick of the clock consisted of sudden movement and

stoppage, it caused minute variation in the rate of subsidence; this

became magnified by the Crescograph and appeared as a series of

oscillations about a mean position of equilibrium. This particular

defect was obviated by the substitution of a fan governor for the

balance wheel. But the speed of rotation slows down with the unwinding

of the main spring, and the balance obtained at the beginning was found

to be insufficient later on. The difficulty was finally overcome by the

use of a heavy weight W, in the place of coiled spring. The complete

apparatus is seen in figure 94.

[Illustration: FIG. 94.--Photographic reproduction of the Balanced

Crescograph. L, L', magnifying compound lever. R, recording plate.

P, plant. C, clock work for oscillation of the plate and lateral

movement. G, governor. M, circular growth-scale. V, plant-chamber.]

For purpose of simplicity of explanation, I assumed the growth rate to

have a definite value of 1/50,000 inch per second. But the rate varies

widely in different plants and even in the same plant at different days

and seasons. In practice the rate of growth for which compensation has

to be made varies from 1/150,000 to 1/25,000 inch, or from 0·17 µ to

1·0 µ per second. We have thus to secure some means of _continuous_

adjustment for growth, the rate of which could be continuously varied

from one to six times. This range of adjustment I have been able to

secure by the compound method of frictional resistance and of

centrifugal governor. As regards frictional resistance the two pointed

ends of a hinged fork rub against a horizontal circular plate not shown

in the figure. By means of the screw head S, the free ends of the fork

spread out and the circumference of the frictional circle continuously

increased. The centrifugal governor is also spread out by the action of

the adjusting screw. By the joint actions of the frictional control and

the centrifugal governor, the speed of rotation can be continuously

adjusted from 1 to 6 times. When the adjusting screw is set in a

particular position, the speed of rotation, and therefore the rate of

subsidence of plant-holder, remains absolutely constant for several

hours. The attainment of this constancy is a matter of fundamental

importance, and it was only by the employment or the compound system of

regulation that I was able to secure it.

The method of obtaining balance now becomes extremely simple. Before

starting the balancing movement by clock regulation, the plant is made

to record its magnified growth by the Crescograph. The compensation is

effected as follows: the speed of the clockwork is at the beginning

adjusted at its lowest value, and the pressure of a button starts the

balancing movement of the plant downwards. On account of partial balance

the record will be found to be less steep than before; the speed of the

clock is gradually increased till the record becomes perfectly

horizontal under exact balance. Overbalance makes the record slope

downwards. In figure 95 is seen records of underbalance (_a_) and

overbalance (_b_), to the extent of about 3 per cent.

[Illustration: FIG. 95.--Balanced Crescographic record: (_a_) showing

effect of underbalance and (_b_) overbalance of about 3 per cent.

(Magnification 2,000 times.)]

It will thus be seen that the effect of an external agent may be

detected by the upsetting of the balance; an up-movement indicates

(unless stated to the contrary) an enhancement of the rate of growth

above the normal; and a down-movement, on the other hand, a depression

of the normal rate.

_Calibration._--The calibration of the instrument is obtained in two

different ways. The rate of subsidence of the plant-holder, by which the

balance is obtained, is strictly proportional to the rate of rotation of

the vertical spindle and the attached train of clock-wheels. A striker

is attached to one of the wheels, and a bell is struck at each complete

revolution. The clockwork is adjusted at a medium speed, the bell

striking 35 times in a minute. A microscope micrometer is focussed on a

mark made on the plant-holder, and the amount of subsidence of the mark

determined after one minute; this was found to be 0·0525 mm. As this

fall occurred after 35 strokes of the bell the subsidence per stroke was

0·0015 mm.

_Determination of the absolute rate of growth._--If growth be found

balanced at N strokes of bell per minute, the rate of subsidence per

second

= N × ·0015/60 mm. per second

= N × ·000025 mm. per second

= N × ·025 µ per second

= N × 10^{-5} inch per second.

_Example._--The growth of a specimen of _Zea Mays_ was found balanced

when the number of strokes of the bell was 20 times in a minute.

Absolute rate of growth = 20 × ·025 µ = 0·5 µ per second

or = 20 × 10^{-5} inch "

or = 1/50,000 " "

If we take the wave length of sodium light [Greek: lambda] as our

standard, the growth in length per second is equal to [Greek: lambda].

This will give us some idea of the sensitiveness of the Crescograph

employed in recording the movement of growth.

GROWTH-SCALE.

The Balanced Crescograph enables us not merely to determine the absolute

rate of growth, but the slightest fluctuation in that rate.

_Indicator Scale._--All necessity of calculation is obviated by the

scale provided with the apparatus. The speed of clockwork which brings

about the balance of growth is determined by the position of the

adjusting screw S, the gradual lowering of which produces a continuous

diminution of speed. A particular position of the screw therefore

indicates a definite rate of subsidence for balancing growth. By a

simple mechanism the up or down movement of the screw causes rotation of

an index pivoted at the centre of a circular scale. Each division of the

scale is calibrated by counting the corresponding number of strokes of

the bell per minute at different positions of the adjusting screw. The

scale is calibrated in this manner to indicate different rates of growth

from 0·2 µ to 1·2 µ per second.

The determination of the rate of growth now becomes extremely simple.

Few turns of the screw bring about the balance of growth and the

resulting position of the index against the circular scale automatically

indicates the absolute rate. The procedure is even simpler and more

expeditious than the determination of the weight of a substance by means

of a balance.

SENSITIVENESS OF THE CRESCOGRAPHIC BALANCE.

Perhaps the most delicate method of measuring lengths is that afforded

indirectly by the spectrum of a light. A good spectroscope resolves

differences of wave lengths of D_{1} ( = 0·5896 µ) and D_{2} ( = 0·5890)

_i.e._ of 1 part in a thousand. The average rate of growth of _Zea Mays_

is of this order; being about 0·5 µ per second. Let us consider the

question of the possibility of detecting a fractional variation of the

ultra-microscopic length by means of the Balanced Crescograph. In

reality the problem before us is more intricate than simple measurement

of change of length; for we have to determine the _rate of variation_ of

length.

The sensitiveness of the balance will, it is obvious, depend on the

magnifying power of the Crescograph. By the Method of Magnetic

Amplification referred to in page 170, I have succeeded in obtaining a

magnification of ten million times. In this method a very delicate

astatic system of magnets undergoes deflection by the movement of a

magnetised lever in its neighbourhood. A spot of light reflected from a

small mirror attached to the astatic system, thus gives the highly

magnified movement of the rate of growth, which may easily be raised to

ten million times. I shall in the following describe the results

obtained with this easily managed magnification of ten million times.

_Determination of sensitiveness: Experiment 99._--A seedling of _Zea

Mays_ was placed on the Crescographic Balance; and the magnetic

amplification, as stated above, was ten million times. With 18 strokes

of the bell per minute the spot of light had a drift of + 266 cm. per

minute to the right; this is because the growth was underbalanced. With

faster rate of clock movement, _i.e._, 21 strokes in 68 seconds or 18·53

strokes per minute, the drift of the spot of light, owing to

overbalance, was to the left at the rate of -530 cm. per minute.

Thus

(1) 18 strokes per minute caused a drift of +266 cm. per minute.

(2) 18·53 strokes per minute caused a drift of -530 cm. per minute.

Hence by interpolation the exact balance is found to correspond to

18·177 strokes per minute.

Therefore the absolute rate of growth

= 18·177 × 0·025 µ per second.

= 0·45 µ per second.

= 0·000018 inch per second.

We learn further from (1) and (2) that a variation of

(18·53 - 18)/18·177 produces a change of drift of the spot of

light from +266 to -530 cm., _i.e._, of 796 cm. per minute.

As it is easy to detect a drift of 1 cm. per minute a variation of

0·53/(18·177 × 796), or 1 part in 27,000 may thus be detected by the

Method of Balance. The spectroscopic method enabled us, as we saw, to

detect change of wave length 1 part in a thousand. The sensibility of

the Balanced Crescograph is thus seen to rival, if not surpass that of

the spectroscope.

For obtaining a general idea of the sensitiveness, the absolute of

growth in the instance given above was 0·00018 inch per second, and the

Balanced Crescograph was shown capable of discriminating a variation

of 1 part in 27,000; hence it is possible to detect by this means a

variation of 1/1,500 millionth of an inch per second.

This method of unprecedented delicacy opens out a new field of

investigation on the effect of changes of environment in modification of

growth; instances of this will be found in subsequent chapters. I give

below accounts of certain demonstrations which will no doubt appear as

very striking.

After obtaining the exact balance a match was struck in the

neighbourhood of the plant. This produced a marked movement of the

hitherto quiescent spot of light, thus indicating the perception of such

an extremely feeble stimulus by the plant.

Breathing on the plant causes an enhancement of growth due to the joint

effects of warmth and carbonic acid gas. A more striking experiment is

to fill a small jar with carbonic acid and empty it over the plant. A

violent movement of the spot of light to the right demonstrates the

stimulating effect of this gas on growth.

The method described above is excessively sensitive; for general

purposes and for the method of direct record, a less sensitive

arrangement is sufficient. I give below accounts of several typical

experiments in which the recording form of Crescograph was employed, the

magnification being only 2,000 times.

[Illustration: FIG. 96.--Record showing the effect of CO_{2}. Horizontal

line at beginning indicates balanced growth. Application of CO_{2} at

arrow induces enhancement of growth shown by the up-curve followed by

depression, shown by the down-curve. Successive dots at intervals of 10

seconds. (Seedling of wheat.)]

_Effect of carbonic acid on Balanced growth: Experiment 100._--I have

already shown that carbonic acid diluted with air induces an enhancement

of the rate of growth, but its long continued action induces a

depression (p. 185). I shall now employ the Method of Balance in

studying the effect of CO_{2} on growth. It should be remembered in this

connection that the horizontal record indicates the balance of normal

rate of growth. An up-curve exhibits the induced enhancement and a

down-curve, a depression of growth. In the present experiment after

obtaining the exact balance, pure carbonic acid gas was made to fill up

the plant-chamber at the point marked with an arrow (Fig. 96). It will

be seen that this induced an almost immediate acceleration of the rate,

the latent period being less than five seconds. The acceleration

continued for two and half minutes; the accelerated rate then slowed

down, became enfeebled, and the growth returned for a short time to the

normal as indicated by the horizontal portion at the top of the record;

this proved to be the turning point of inversion from acceleration into

retardation of growth. The stronger is the concentration of the gas the

earlier is the point of inversion. With diluted carbonic acid the

acceleration may persist for an hour or more.

EFFECT OF ANÆSTHETICS.

_Effect of Ether: Experiment 101._--Dilute vapour of ether is found to

induce an acceleration of rate of growth which persist for a

considerable length of time. This is seen in the upsetting of the

balance upwards on the introduction of the vapour (Fig. 97a.).

[Illustration: FIG. 97.--(_a_) Effect of ether, acceleration of growth,

(_b_) effect of chloroform preliminary acceleration followed by

depression.]

_Effect of Chloroform: Experiment 102._--The effect of chloroform vapour

is relatively more depressing than ether. Application of chloroform is

seen to induce at first an acceleration which persisted for 50 seconds,

but after this depression set in (Fig. 97b). Prolonged application of

the anæsthetic is followed by the death of the plant.

SUMMARY.

In the Method of Balance the movement of growth upwards is compensated

by an equal movement of the plant downwards, with the result that the

record remains horizontal.

The effect of an external agent is immediately detected by the upsetting

of the balance, up-record representing acceleration above normal, a

down-record the opposite effect of depression below the normal rate.

The latent period and the after-effect of stimulus may thus be obtained

with the highest accuracy.

The sensitiveness of the Method of Balance may be raised so as to

indicate a variation of rate of growth smaller than 1/1000 millionth of

an inch per second.

XXIII.--ON TROPIC MOVEMENTS

_By_

SIR J. C. BOSE.

The diverse movements induced by external stimuli in different organs of

plants are extremely varied and complicated. The forces in operation are

manifold--the influence of changing temperature, the stimulus of

contact, of electric current, of gravity, and of light visible and

invisible. They act on organs which exhibit all degrees of physiological

differentiation, from the radial to the dorsiventral. An identical

stimulus may sometimes induce one effect, and at other times, the

precisely opposite. Thus under unilateral stimulation of light of

increasing intensity, a radial organ exhibits a positive, a

dia-phototropic, and finally a negative response. Strong sunlight brings

about para-heliotropic or 'midday sleep' movement, by which the apices

of leaves or leaflets turn towards or away from the source of

illumination. The teleological argument advanced, that in this position

the plant is protected from excessive transpiration, does not hold good

universally; for under the same reaction, the leaflets of _Cassia

montana_ assume positions by which the plant risks fatal loss of water.

In _Averrhoa carambola_ the movement is downwards, whichever side is

illuminated with strong light; in _Mimosa_ leaflet the movement, under

similar circumstances is precisely in the opposite direction. The

photonastic movement, apparently independent of the directive action of

light, has come to be regarded as a phenomenon unrelated to phototropic

reaction, and due to a different kind of irritability, and a different

mode of response. So very anomalous are these various effects that

Pfeffer, after showing the inadequacy of different theories that have

been advanced, came to the conclusion that "the precise character of the

stimulatory action of light has yet to be determined. When we say that

an organ curves towards a source of illumination because of its

heliotropic irritability, we are simply expressing an ascertained fact

in a conveniently abbreviated form, without explaining why such

curvature is possible or how it is produced."[2]

[2] Pfeffer--_Ibid_--Vol. II, p. 74.

The contradictory nature of the various responses is however not real;

the apparent anomaly had lain in the fact that two definite fundamental

reactions of opposite signs induced by stimulus had not hitherto been

recognised and distinguished from each other. The innumerable variations

in the resultant response are due to the summation of the effects of two

fluctuating factors, with further complications arising from: (1)

difference in the point of application of stimulus, (2) the differential

excitability of the different sides of the responding organ, and (3) the

effect of temperature in modifying tropic curvature. It is therefore

most important to have the means for automatic record of _continuous_

change in the response brought about by various factors, which act

sometimes in accord, and at other times in conflict. The autograph of

the plant itself, giving a history of the change in response and its

time-relations, is alone decisive in explanation of various difficulties

in connection with plant movements, as against the various tentative

theories that have been put forward. The analysis of the resulting

effect, thus rendered possible, casts new light on the phenomena of

response, proving that the anomalies which had so long perplexed us, are

more apparent than real.

One of the causes of uncertainty lay with the question, whether response

changed with the mode of stimulation. I have, however, been able to show

that _all forms of stimuli_ induce a definite excitatory reaction of

contraction (p. 218).

Tropic movements induced by unilateral action of stimulus may, broadly

speaking, be divided into two classes depending on the point of

application of stimulus:

In the first, the point of application of unilateral stimulus is not on

the responding organ itself, but at some distance from it. The question

therefore relates to LONGITUDINAL TRANSMISSION of effect of stimulus.

In the second, unilateral stimulus acts directly on the responding

organ. For the determination of the resultant movement, it is necessary

to take account of effects induced on the two sides of the organ. The

side adjacent to the stimulus I shall designate as the _proximal_, and

the diametrically opposite as the _distal_ side. The question to be

investigated in this case relates to TRANSVERSE TRANSMISSION of effect

of stimulus. It will be shown that the resulting movement depends on:--

(_a_) whether the tissue is a conductor or a non-conductor of

excitation in a transverse direction, and

(_b_) whether it is the proximal, or the distal side of the

organ that is the more excitable.

In connection with the response to environmental changes, a source of

uncertainty is traceable to the absence of sufficient knowledge of the

physiological effect of heat, which has been regarded as a form of

stimulus: it will be shown that heat induces two distinct effects

dependent on conduction and radiation. We shall in the succeeding

chapters, take up the study of the physiological effects induced by

changes in the environment.

XXIV.--TROPIC CURVATURE WITH LONGITUDINAL TRANSMISSION OF EFFECT OF

STIMULUS

_By_

SIR J. C. BOSE,

_Assisted by_

GURUPRASANNA DAS.

I have in previous chapters explained that the direct application of

stimulus gives rise in different organs to contraction, diminution of

turgor, fall of motile leaf, electro-motive change of galvanometric

negativity, and retardation of the rate of growth. I have also shown

that indirect stimulation (_i.e._ application of stimulus at some

distance from the responding organ) gives rise to a positive or erectile

response of the responding leaf or leaflet (indicative of an increase of

turgor), often followed by normal negative response. The positive

impulse travels quickly. The interval of time that elapses, between the

application of stimulus and the erectile response of the responding

leaf, depends on the distance of the point of application, and the

character of the transmitting tissue: it varies in different cases from

0·6 second to about 40 seconds. The positive is followed by a slower

wave of protoplasmic excitation, which causes the excitatory fall. The

velocity of this excitatory impulse is about 30 mm. per second in the

petiole of _Mimosa_, and about 3 mm. per second in _Biophytum_. The

positive followed by the negative thus gives rise to a diphasic

response. The excitatory impulse is much enfeebled during transit: the

negative impulse may thus fail to reach the responding organ, if the

stimulus be feeble or if the intervening distance be long or

semi-conducting. Hence moderate stimulus applied at a distance gives

rise only to positive response; direct application of strong stimulus

gives rise, on the other hand, to the normal negative. By employing the

electric method of investigation, I have obtained with ordinary tissues

the positive, the diphasic, and the negative electric response, in

correspondence with the responses given by a motile organ (p. 214). The

mechanics of propagation of the positive and the negative impulse are

different. It is therefore necessary to distinguish the quick

_transmission_ of the positive impulse from the slow _conduction_ of the

negative impulse due to the propagation of excitatory protoplasmic

change.

It should be borne in mind in this connection that all responsive

movements are ultimately due to protoplasmic changes which are beyond

our scrutiny. We can infer the nature of the change by the concomitant

outward manifestations, which are of two kinds: the _positive_,

associated with increase of turgor, expansion, and galvanometric

positivity, and the _negative_ with concomitant decrease of turgor,

contraction, and galvanometric negativity. Thus positive and negative

reactions indicate the fundamental protoplasmic changes of opposite

characters.

The movement and curvature induced by stimulus have, for convenience,

been distinguished as _positive curvature_, (movement towards stimulus),

and _negative curvature_ (movement away from stimulus). Though these

curvatures result from protoplasmic reactions, yet the _positive

curvature_ is not necessarily associated with _positive protoplasmic

reaction_. It will be shown that the curvature of an organ is determined

by the algebraical summation of effects induced at the proximal and

distal sides of the responding organ.

Physiologists have not been aware of the dual character of the impulse

generated by stimulus, and the term "transmission of stimulus" is thus

misleading since its effect may be an expansion, or its very opposite,

contraction. It is therefore necessary to discriminate the effect of one

from the other: the impulse which induces an increase of turgor,

expansion, and galvanometric positivity will be distinguished as

positive, in the sense that it causes an enhancement of turgor. The

other, which induces diminution of turgor and contraction, will be

termed as the excitatory impulse. Transmission of the latter is

dependent on conducting power of the tissue; the positive impulse is

practically independent of the conducting power.

In animal physiology again, there is no essential difference between the

effect of the direct and indirect stimulation. In a nerve-and-muscle

preparation, for example, indirect stimulation at the nerve induces the

same contraction as the direct stimulation of the muscle. The only

difference lies in the latent period, which is found to be longer under

indirect stimulation by the time interval necessary for the excitation

to travel along the conducting nerve. It is probable that stimulus gives

rise to dual impulses in the animal tissue as in the plant. But the

detection of the positive impulse in the animal nerve is rendered

exceedingly difficult on account of the high velocity of conduction of

excitation. I have explained that the separate effects of the two

impulses can only be detected if there is a sufficient lag of the

excitatory negative behind the positive, so that the relatively sluggish

responding organ may exhibit the two impulses one after the other. In a

highly conducting tissue the lag is very slight, and the negative will

therefore mask the positive by its predominant effect. In spite of the

difficulty involved in the problem, I have recently been successful in

demonstrating the dual impulses in the animal nerve.

In any case it is important to remember the following characteristic

effects of indirect stimulation.

TABLE XXII.--SHOWING THE EFFECT OF INDIRECT STIMULATION.

+-----------------------------------------------------------------+

| Intensity of | Character of intervening | Responsive effect. |

| Stimulus. | tissue. | |

+-----------------+--------------------------+--------------------+

|Moderate |Highly Conducting | Contraction. |

| " |Non-conducting | Expansion. |

| " |Semi-conducting | Expansion followed |

| | | by contraction. |

|Feeble | " " | Expansion. |

+-----------------------------------------------------------------+

These effects of indirect stimulation have been fully demonstrated in

the case of pulvinated organs (p. 136) and growing organs (p. 215).

Having demonstrated the fundamental reactions of direct and indirect

stimulation, we shall next study the tropic effects induced in growing

organs by the effect of unilateral application of indirect stimulus.

_Experiment 103._--I have already explained, how thermal _radiation_ is

almost as effective in inducing contraction and retardation of growth as

the more refrangible rays of the spectrum. The thermal radiation was

produced by the heating of a platinum spiral, short of incandescence, by

the passage of an electric current. The intensity of radiation is easily

varied by adjustment of the current by means of a rheostat. The

experimental specimen was a flower bud of _Crinum_. It was held by a

clamp, a little below the region of growth. Stimulus was applied below

the clamp so that the transmitted effect had to pass through S, the

securely held tissue (Fig. 98). A feeble stimulus was applied on one

side, at the indifferent point about 3 cm. below the region of growth.

The positive effect of indirect stimulus reached the region of growth on

the same side, bringing about an acceleration of growth with expansion

and convexity, the resulting movement being _negative_ or away from the

stimulus. The latent period was ten seconds, and maximum negative

movement was completed in the further course of ten seconds, after which

there was a recovery in the course of 75 seconds. A stronger stimulus S'

gave a larger response; but when the intensity was raised still higher

to S", the excitatory negative impulse overtook the positive within 15

seconds of its commencement; the convex was thus succeeded by the

concave curvature (Fig. 99). Direct application of stimulus at the

growing region gave rise to a positive curvature.

[Illustration: FIG. 98.--Diagrammatic representation of effects of

indirect and direct stimulation. Continuous arrow represents the

indirect stimulation, and the curved continuous arrow above, the induced

negative curvature: dotted arrow indicates the application of direct

stimulus, and the dotted curve above, the induced positive curvature.]

[Illustration: FIG. 99.--Tropic curvature of _Crinum_ to unilateral

indirect stimulation of increasing intensities: S, S' of moderate

intensity induced negative tropic effect (movement away from the

stimulated side); stronger stimulus S" gave rise to negative followed by

positive. Successive dots at intervals of 5 seconds Magnification 100

times.]

The effect of feeble stimulus transmitted longitudinally is thus found

always to induce convexity, a _negative curvature_ and movement away

from stimulus. I have obtained similar responsive movement of negative

sign with various plant organs, and under various forms of stimuli. Thus

in the stem of _Dregea volubilis_ the longitudinally transmitted effect

of light of moderate intensity was a negative curvature; direct

application of light on the growing region gave, on the other hand, a

positive curvature and movement towards light.

Thus while the effect of direct unilateral stimulation is a positive

curvature, the effect of indirect stimulation is a negative curvature.

The following table gives a summary of results of tropic effects under

unilateral application of indirect stimulus.

TABLE XXIII.--SHOWING TROPIC EFFECT OF UNILATERAL APPLICATION OF

INDIRECT STIMULUS.

+------------------------------------------------------------+

|Stimulus. | Character of intervening | Sign of tropic |

| | tissue. | response. |

+----------+---------------------------+---------------------+

| Moderate | Conducting | Positive curvature. |

| " | Semi-conducting | Negative followed |

| | | by positive. |

| Feeble | Semi-conducting | Negative Curvature. |

| Moderate | Non-conducting | " " |

+----------+---------------------------+---------------------+

|Direct application of unilateral stimulus induces a positive|

|curvature. |

+------------------------------------------------------------+

SUMMARY.

In sensitive plants stimulus applied at a distance induces in the

responding region an expansion indicative of increase of turgor.

The effect of indirect stimulation is also exhibited by an electric

change of galvanometric positivity, indicative of enhancement of turgor

and expansion.

Indirect stimulus induces in growing organs an enhancement of rate of

growth.

Unilateral application of stimulus causes an expansion higher up on the

same side to which the stimulus is applied; the result is an induced

convexity, a movement away from the stimulus, _i.e._, a negative

curvature. Direct stimulus applied unilaterally at the responding region

induces, on the other hand, a positive curvature.

XXV.--TROPIC CURVATURE WITH TRANSVERSE TRANSMISSION OF EFFECT OF

STIMULUS

_By_

SIR J. C. BOSE,

_Assisted by_

GURUPRASANNA DAS.

We have next to consider a very large class of phenomena arising out of

the direct stimulation of one side and its transversely transmitted

effect on the opposite side. The unilateral stimuli to which the plant

is naturally exposed are those of contact, of light, of thermal

radiation, and of gravity. There is besides the stimulation by electric

current. I shall presently show that these tropic curvatures are

determined by the definite effects of direct and indirect stimulations.

Under unilateral stimulus, the proximal side is found to become concave

and the distal side convex; the organ thus moves towards stimulus,

exhibiting a positive curvature. This movement may be due: (1) to the

diminution of turgor, contraction or retardation of rate of growth of

the proximal side, (2) to the increase of turgor, expansion or

acceleration of rate of growth on the distal side, or (3) to the joint

effects of contraction of the proximal and expansion of the distal side.

As regards the reaction of the proximal side, it has been shown that

direct stimulation induces local contraction in a pulvinated organ, and

retardation of growth in a growing organ. The effect induced on the

distal side had hitherto remained a matter of uncertainty. In regard to

this we must bear in mind that it is the effect of indirect stimulus

that reaches the distal sided, inducing an enhancement of turgor and

expansion of that side.

For obtaining a complete explanation of tropic curvatures in general, it

is important that the induction of enhanced turgor at the distal side

(by the action of stimulus at the proximal side) should be corroborated

by independent methods of enquiry. One of the methods I employed for

this purpose was electrical. Two electric connections were made, one

with the distal point (diametrically opposite to the stimulated area),

and the other, with an indifferent point at a distance. On application

of stimulus of various kinds, the distal point was found to exhibit

galvanometric positivity, indicative of enhancement of turgor.[3]

[3] "Plant Response"--p. 519.

I have since been able to devise a new experiment by which the

enhancement of turgor on the distal side is demonstrated in a very

striking manner.

I have shown (p. 39) that the movement of the motile leaf of _Mimosa_ is

a reliable indicator of the state of turgor, increase of turgor inducing

erection, and diminution of turgor bringing about the fall of the leaf.

I shall employ the mechanical response of the leaf to demonstrate the

enhancement of turgor induced by transverse transmission of effect of

stimulus.

[Illustration: FIG. 100.--Increased turgor due to indirect stimulation,

inducing erection of Mimosa leaf: (_a_) diagram of the experiment, point

of application of stimulus indicated by arrow. (_b_) erectile response

(shown by down-curve) followed by rapid fall (up-curve) due to

transverse conduction of true excitation. (Successive dots at intervals

of 10 seconds.)]

TURGOR-VARIATION UNDER TRANSVERSE TRANSMISSION OF STIMULUS-EFFECT.

_Unilateral photic stimulation: Experiment 104._--A _Mimosa_ plant was

taken, and its stem was held vertical by means of a clamp. We apply a

stimulus at a point on one side of the stem, and observe the effect of

this on the state of turgor at the diametrically opposite side. In my

first experiment on the subject of detection of induced change of

turgor I employed the stimulus of light. A narrow beam from a small arc

lamp was made to fall on the stem, at a point diametrically opposite to

the motile leaf, which was to serve as a indicator for induced variation

of turgor at the distal side. The leaf was attached to the recording

lever, the successive dots in the record being at intervals of ten

seconds. Stimulation by light caused a positive or erectile movement

within 20 seconds of application. The positive response afforded a

conclusive proof of the induction of an increase of turgor at the distal

point. When the stimulus is moderate or of short duration, the response

remains positive. But with strong or prolonged stimulation, the slower

excitatory negative impulse is conducted to the distal point and brings

about the sudden fall of the leaf (Fig. 100). In the present case the

excitatory impulse reached the motile organ 200 seconds after the

initiation of the positive response. The stem was thin, only 2 mm. in

diameter. The velocity of excitatory impulse in a transverse direction

is thus 0·01 mm. per second; transverse transmission is, for obvious

reasons, a much slower process than longitudinal transmission of

excitation; in the _Mimosa_ stem this is about 4 mm. per second.

[Illustration: FIG. 101.--Response of leaf of _Mimosa_ under transverse

transmission of electric stimulus. (Compare this with fig. 100.)]

_Unilateral electric stimulation: Experiment 105._--In order to show

that the effects described above are not due to any particular mode of

stimulation but to stimuli in general, I carried out an additional

experiment, the stimulus employed being electrical. Two fine

pin-electrodes were pricked into the stem, opposite to the responding

leaf of _Mimosa_; these electrodes were placed vertically one above the

other, 5 mm. apart. After a suitable period, allowed for recovery from

mechanical irritation, feeble tetanising electric shock was passed

through the electrodes. The responsive effects at the distal side of the

stem is precisely similar to those induced under unilateral photic

stimulation; that is to say, the first effect was an erectile movement

of the leaf, indicative of an induced enhancement of turgor; the

excitatory negative impulse then reached the distal point and caused a

sudden fall of the leaf (Fig. 101).

The experiments that have just been described are of much significance.

An organ like the stem of _Mimosa_, since it exhibits no contraction,

may appear insensitive to stimulation; but its perception of stimulus is

shown by its power of transmitting two characteristic impulses, one of

which is the positive, giving rise to an enhancement of turgor, and the

other, the true excitatory negative, inducing the opposite reaction or

diminution of turgor. Unilateral stimulation gives rise to both these

effects in all organs: pulvinated, growing, and non-growing. It was the

fortunate circumstance of the insertion of the motile leaf on one side

of the _Mimosa_ stem that enabled us to demonstrate the important facts

given above.

The underlying reactions, which give rise to tropic curvature, could

have been foretold from the Laws of effects of Direct and Indirect

stimulation, established in previous chapters (pp. 136, 216). The

resulting curvature is thus brought about by the joint effects of direct

stimulation of the proximal, and indirect stimulation of the distal

side. We may now recapitulate some of the important facts relating to

tropic curvatures:

Indirect stimulation gives rise to dual impulses, positive and negative;

of these the positive impulse is practically independent of the

conducting power of the tissue; but the transmission of the excitatory

negative impulse is dependent on the conducting power. No tissue is a

perfect conductor, nor is any a perfect non-conductor of excitation, the

difference is a question of degree. In a petiole or a stem the

conducting power along the direction of length is considerable, but very

feeble in a transverse direction. In a semi-conducting tissue, a feeble

stimulus will transmit only the positive impulse; strong or long

continued stimulation will transmit both positive and negative impulses,

the positive preceding the negative. The transmitted positive gives rise

to increase of turgor, expansion, and acceleration of rate of growth;

the negative induces the opposite reaction of diminution of turgor, of

contraction, and of retardation of rate of growth. Transverse

transmission is only a particular instance of transmission in general;

the only difference is that the conducting power for _excitation_ is

very much less in the transverse than in the longitudinal direction.

Owing to feeble transverse conductivity, the transmitted impulse to the

distal side often remains positive; it is only under strong or continued

stimulation that the excitatory negative reaches the distal side and

neutralises or reverses the previous positive reaction. If the distal is

the more excitable side, the reversed response will appear as pronounced

negative. I give a table which will clearly exhibit the effects of

stimulus on the proximal and distal sides of the responding organ.

TABLE XXIV.--SHOWING RESPONSIVE EFFECTS COMMON TO PULVINI AND GROWING

ORGANS UNDER UNILATERAL STIMULATION.

+------------------------------------------------------------------+

|Effect of direct stimulation on | Effect of indirect stimulation |

| proximal side. | on distal side. |

+---------------------------------+--------------------------------+

|Diminution of turgor | Increase of turgor. |

|Galvanometric negativity | Galvanometric positivity. |

|Contraction and concavity | Expansion and convexity. |

+------------------------------------------------------------------+

| When stimulus is strong or long continued, the |

| true excitatory effect isconducted to the |

| distal side, neutralising or reversing the first response. |

+------------------------------------------------------------------+

The diagram which I have already given (Fig. 98) clearly explains the

different tropic effects induced by changing the point of application of

stimulus. We may thus have stimulus applied at the responding region

itself (Direct Stimulation) or at some distance from it (Indirect

Stimulation). The final effect will be modified by the conducting power

of the tissue.

DIRECT UNILATERAL STIMULATION.

_Type I._--The tissue has little or no power of transverse

conduction: stimulus remains localised, the proximal side

undergoes contraction, and the distal side expansion. The

result is a positive curvature.

_Type II._--The tissue is transversely conducting. Under

strong and long continued stimulation the excitatory impulse

reaches the distal side, neutralising or reversing the first

effect.

INDIRECT UNILATERAL STIMULATION.

_Type I._--The intervening tissue is an indifferent

conductor: transmitted positive impulse induces expansion and

convexity on the same side, thus giving rise to negative

curvature (_i.e._, away from stimulus).

_Type II._--Intervening tissue is a fairly good conductor:

the effect of positive impulse is over-powered by the

predominant excitatory negative impulse, the final result is

a concavity and positive curvature, with movement towards the

stimulus.

The following is a tabular statement of the different effects induced by

Direct and Indirect stimulation.

TABLE XXV.--SHOWING DIFFERENCE OF EFFECTS INDUCED BY DIRECT AND INDIRECT

STIMULATION.

+------------------------------------------------------------------+

|Stimulation. |Nature of the tissue. |Final effect. |

+---------------+----------------------------+---------------------+

|Direct (Feeble)|Semi-conducting tissue. |Positive curvature. |

|Indirect " | " " |Negative curvature. |

|Direct (Strong)|Better conducting tissue. |Neutral or negative |

| | |curvature. |

|Indirect " | " " " |Negative followed by |

| | |positive curvature. |

+------------------------------------------------------------------+

The results of investigations already described, enable us to formulate

the general laws of tropic curvature applicable to all forms of stimuli,

and to all types of responding organs, pulvinated or growing.

LAWS OF TROPIC CURVATURE.

1. (_a_) DIRECT APPLICATION OF UNILATERAL STIMULUS OF

MODERATE INTENSITY, INDUCES A POSITIVE OR CONCAVE CURVATURE,

BY THE CONTRACTION OF THE PROXIMAL AND EXPANSION OF THE

DISTAL SIDE.

(_b_) UNDER STRONG OR LONG-CONTINUED STIMULATION, THE

POSITIVE CURVATURE IS NEUTRALISED OR REVERSED, BY TRANSVERSE

CONDUCTION OF EXCITATION; THIS EFFECT IS ACCENTUATED BY THE

DIFFERENTIAL EXCITABILITY OF THE TWO SIDES OF THE ORGAN.

2. (_a_) INDIRECT APPLICATION OF UNILATERAL STIMULUS OF

FEEBLE INTENSITY INDUCES A NEGATIVE CURVATURE.

(_b_) IN A CONDUCTING TISSUE THE EXCITATORY EFFECT BEING

TRANSMITTED UNDER STRONG AND LONG CONTINUED STIMULATION,

INDUCES A POSITIVE CURVATURE.

It will thus be seen that the tropic effect is modified by:

(1) the point of application of stimulus,

(2) the intensity and duration of stimulus,

(3) the conducting power of tissue in the transverse

direction,

(4) the relative excitabilities of the proximal and distal

sides of the organ.

In the following series of Papers the tropic effects of various forms of

stimuli will be studied in detail.

SUMMARY.

In a semi-conducting tissue Direct stimulation induces a diminution of

turgor and contraction, Indirect stimulation inducing the opposite

effect of increase of turgor and expansion.

Unilateral stimulation thus induces a positive curvature by the joint

effects of contraction at the proximal, and expansion at the distal

side.

Under strong and long continued unilateral stimulation, the excitation

at the proximal side is transmitted to the distal side. Transverse

conduction thus neutralises or reverses the normal positive curvature.

XXVI.--MECHANOTROPISM: TWINING OF TENDRILS

_By_

SIR J. C. BOSE,

_Assisted by_

GURUPRASANNA DAS.

In response to the stimulus of contact a tendril twines round its

support. Certain tendrils are uniformly sensitive on all sides; but in

other cases, as in the tendril of _Passiflora_, the sensitiveness is

greater on the under side. A curvature is induced when this side is

rubbed with a splinter of wood, the stimulated under side becoming

concave. This movement may be distinguished as a movement of _curling_.

There is, as I shall presently show, a response where the under side

becomes convex, and the curvature becomes reversed.

As regards perception of mechanical stimulus, Pfeffer discovered tactile

pits in the tendrils _Cucurbitaceæ_. These pits no doubt facilitate

sudden deformation of the sensitive protoplasm by frictional contact. No

satisfactory explanation has however been offered as regards the

physiological machinery of responsive movement. The difficulty of

explanation of twining movements is accentuated by a peculiarity in the

response of tendrils which is extremely puzzling. This anomaly was

observed by Fitting in tendrils which are sensitive on the under side:

"If a small part of the upper side and at the same time the

whole of the under side be stimulated, curvature takes place

only at the places on the under side which lie opposite

to the unstimulated regions of the upper side. The

_sensitiveness_ to contact is thus as well developed on the

upper side as on the under side, and the difference between

the two sides lies in the fact that while stimulation of the

under side induces curvature, stimulation of the upper side

induces _no visible result_, or simply inhibits curvature on

the under side, according to circumstances."[4]

[4] Jost--_Ibid_--p. 490.

Here then we have the inexplicable phenomenon of a particular tissue,

itself incapable of response, yet arresting the movement in a

neighbouring tissue.

The problem before us may be thus stated: Is the movement of the tendril

due to certain specific sensibility of the organ, on account of which

its reactions are characteristically different from other tropic

movements? Or, does the twining of tendril come under the law of tropic

curvature that has been established, namely that it is brought about by

the contraction of the directly stimulated proximal side, and the

expansion of the indirectly stimulated distal side?

I shall now describe my investigations on the effects of direct and

indirect stimulus on the growth of tendril; I have in this

investigation studied the effect not merely of mechanical, but also of

other forms of stimuli. I shall also describe the diverse effects

induced by mechanical stimulus under different conditions. From the

results of these experiments I shall be able to show that the twining of

the tendril comes under the general law of tropic curvature; that the

curvature results from the contraction of the proximal and expansion of

the distal side. Finally I shall be able to offer a satisfactory

explanation of the inhibition of response of the tendril by the

stimulation of the opposite side of the organ.

GENERAL EFFECTS OF INDIRECT AND DIRECT ELECTRIC STIMULATION ON THE

GROWTH OF TENDRIL.

For this experiment I took a growing tendril of _Cucurbita_ in which the

sensitiveness is more or less uniform on all sides. The tendril was

suitably mounted on the Balanced Crescograph, which records the

variation of the rate of growth induced by immediate and after-effect of

stimulus. The specimen is held in a clamp as in the diagram (Fig. 102),

the tip being suitably attached to the recording lever. For indirect

stimulation feeble shock from an induction coil is applied at the two

electric connections below the clamp. Direct stimulus is applied by

means of electric connections one above and the other below the clamp.

[Illustration: FIG. 102.--Diagrammatic representation of indirect and

direct stimulation of tendril.]

_Effect of Indirect Stimulus: Experiment 106._--The growth of the

tendril was exactly balanced, and the record became horizontal. Indirect

stimulus was next applied below the clamp; this is seen to upset the

balance, with the resulting up-curve which indicates a sudden

acceleration of growth above the normal. This acceleration took place

within ten seconds of the application of stimulus, and persisted for

three minutes; after this the normal rate of growth became restored, as

seen by the balanced record once more becoming horizontal (Fig. 103).

[Illustration: FIG. 103.--Record by Method of Balance, showing

acceleration of growth of tendril (up-curve) induced by indirect

stimulation. (_Cucurbita._)]

_Effect of Direct Stimulus: Experiment 107._--The incipient contraction

induced by direct stimulation is so great that the record obtained by

the delicate method of balance cannot be kept within the plate. I,

therefore, took the ordinary growth-curve on a moving plate. The first

part of the curve represents normal growth; stimulus of feeble electric

shock was applied at the highest point of the curve. This is seen (Fig.

104) to induce an immediate contraction and reversal of the curve which

persisted for two and half minutes, after which growth was slowly

renewed. The most interesting fact regarding the after-effect of

stimulus is that the rate of growth became actually enhanced to three

times the normal. This is clearly seen in the record (upper half of the

figure) taken 20 minutes after stimulation, where the curve is far more

erect than that of the normal rate of growth before stimulation.

[Illustration: FIG. 104.--Variation of growth induced by direct

stimulation. First part of the curve shows normal rate of growth. Direct

stimulation induces contraction (reversal of curve). After-effect of

stimulus seen in highly erect curve in upper part of record, taken 20

minutes after.]

The effects of Indirect and Direct stimulation of the tendril are

summarised below:

(1) Indirect stimulation induces a sudden enhancement of rate

of growth, followed by a recovery of the normal rate.

(2) Direct stimulation induces a retardation of the rate of

growth which may culminate into an actual contraction. _The

after-effect of direct stimulus of moderate intensity is an

enhancement of the rate of growth._

The experiments described above demonstrate the effects of direct and

indirect electrical stimulus. I shall now proceed to show that

mechanical stimulus induces effects which are similar to those of

electric stimulus.

EFFECTS OF DIRECT AND INDIRECT MECHANICAL STIMULUS.

_Effect of Direct mechanical stimulus: Experiment 108._--In this case I

took a tendril of _Cucurbita_, and attached it to the ordinary High

Magnification Crescograph, the record of which gives the absolute rate

of its normal growth, and the induced variation of that rate. The

tendril was stimulated mechanically by simultaneous friction of its

different sides. The immediate effect was a retardation of growth, the

reduced rate being less than half the normal. There was a recovery on

the cessation of the stimulus; the rate of growth was even slightly

enhanced after an interval of 15 minutes. Table XXVI shows the immediate

and after-effects of mechanical stimulation on growth.

TABLE XXVI.--SHOWING THE IMMEDIATE AND AFTER-EFFECT OF MECHANICAL

STIMULATION ON TENDRIL (_Cucurbita_).

+--------------------------------------------------------------+

|Normal rate of growth 0·44 µ per sec. |

|Retarded rate immediately after stimulation 0·20 µ " " |

|Recovery and enhancement after 15 minutes 0·50 µ " " |

+--------------------------------------------------------------+

The immediate and after-effects of mechanical stimulus on the tendril

are therefore the same as that of electric stimulus. The incipient

contraction under direct mechanical stimulus, moreover, is not the

special characteristic of tendrils, but of growing plants in general.

For I have shown (page 203) that the growth of flower stalk of

_Zephyranthes_ is also retarded after mechanical friction, from the

normal rate 0·48 µ to 0·11 µ after stimulation. We shall find later that

different plant organs, after moderate stimulation, exhibit acceleration

of growth as an after-effect. The phenomenon of responsive reaction of

tendril is therefore not unique, but similar to that of other organs

under all forms of stimulation. The only speciality in tendril is that

owing to anatomical peculiarities, the perceptive power of the organ for

mechanical stimulus is highly developed.

We are now in a position to offer an explanation of the induced

concavity of the stimulated side of the tendril, and its recovery after

brief contact. The experiments that have been described show that:

(1) the proximal side contracts because it is directly stimulated,

and the distal side, being indirectly stimulated, expands; the

curvature is thus due to the joint effects of contraction of one

side, and expansion of the opposite side, and

(2) the recovery of the tendril after brief contact is hastened by

the after-effect of stimulus, which is expansion and acceleration

of growth.

The results given above will also be found to explain Fitting's

important observations[5] that (_a_) the stimulated side of the tendril

undergoes transient contraction with subsequent acceleration of growth,

and that (_b_) the distal or convex side undergoes an immediate

enhancement of growth.

[5] Pfeffer--_Ibid_--Vol. III, p. 57.

I give below a record given by a tendril of _Cucurbita_ in response to

unilateral contact of short duration (Fig. 105). Successive dots in the

record are at intervals of three seconds. The latent period was ten

seconds, and the maximum curvature was attained in the course of two and

a half minutes. The curvature persisted for a further period of two

minutes after which recovery was completed in the course of 12 minutes.

Feeble stimulation is attended by a recovery within a short period, but

under strong stimulus the induced curvature becomes more persistent.

[Illustration: FIG. 105.--Positive curvature of tendril of Cucurbita

under unilateral stimulus of contact at x.]

INHIBITORY ACTION OF STIMULUS.

I have referred to the remarkable observation of Fitting that though

the application of stimulus on the upper side of the tendril of

_Passiflora_ did not induce any response, yet it inhibited the normal

response of the under side.

The results of experiments which I have described will, however, afford

a satisfactory explanation of this curious inhibition. It has been

explained, that the curvature of the tendril is due to the joint effects

of diminished turgor and contraction at the directly stimulated side,

and an enhancement of turgor and expansion on the opposite side. In the

diagram seen in figure 106, the left is the more excitable side, and

contraction will induce concavity of the stimulated side. But if the

opposite or less excitable side of the tendril be stimulated at the same

time, then the transmitted effect of indirect stimulus will induce

enhancement of turgor and expansion on the left side, and thus

neutralise the previous effect of direct stimulus. An inhibition of

response will thus result from the stimulation of the opposite side.

[Illustration: FIG. 106.--Diagrammatic representation of effects of

Indirect and Direct unilateral stimulation of the tendril. Indirect

stimulation, I, induces movement away from stimulated side (negative

curvature) represented by continuous arrow. Direct stimulation, D,

induces movement towards stimulus (positive curvature) indicated by

dotted arrow.]

A difficulty arises here from the fact that the upper side of the

tendril (the right side in Fig. 106) is supposed to be inexcitable and

non-contractile. Hence there may be a misgiving that the stimulation of

the non-motile side may not induce the effect of indirect stimulus (an

increase of turgor and expansion) at the opposite side, which is to

inhibit the response. But I have shown that even a non-contractile organ

under stimulus generates both the impulses, positive and negative. This

is seen illustrated in figure 100, where the rigid stem of _Mimosa_ was

subjected to unilateral stimulation; the effect of indirect stimulus was

found to induce an enhancement of turgor at the diametrically opposite

side, and thus caused an erectile movement of the motile leaf. Electric

investigations which I have carried out also corroborate the results

given above. Here also stimulation of a non-motile organ at any point,

induces at a diametrically opposite point, a positive electric variation

indicative of enhanced turgor. It will thus be seen that inhibition is

possible even in the absence of contraction of the upper side of the

tendril; hence the contraction of the directly stimulated side is

neutralised by the effect of indirect stimulation of the distal side.

RESPONSE OF LESS EXCITABLE SIDE OF THE TENDRIL.

It is generally supposed that the upper side of the tendril of

_Passiflora_ is devoid of contractility. This is however not the case,

for my experiments show that stimulation of the upper side also induces

contraction and concavity of that side, though the actual movement is

relatively feeble.

_Experiment 109._--In order to subject the question to quantitative test

I applied feeble stimulus of the same intensity on upper and lower side

alternately. Successive stimuli were kept more or less uniform by

employing the following device. I took a flat strip of wood 1 cm. in

breadth, and coated 2 cm. of its length with shellac varnish mixed with

fine emery powder. On drying the surface became rough, the flat surface

was gently pressed against the area of the tendril to be stimulated, and

quickly drawn so that the rough surface 2 cm.×1 cm. was rubbed against

the tendril in each experiment. Stimulation, thus produced, induced a

responsive movement of each side of the organ. The extent of the

maximum movement was measured by the microscope micrometer. The

following results were obtained with four different specimens.

TABLE XXVII.--SHOWING THE RELATIVE INTENSITIES OF RESPONSES OF THE UPPER

AND UNDER SIDE OF TENDRIL (_Passiflora_).

+------------------------------------------------------------+

|Movement induced by | Movement induced by | B |

| stimulation of under | stimulation of upper | Ratio ---. |

| side, A. | side, B. | A |

+----------------------+-------------------------------------+

|(1) 85 divisions | 14 divisions | 1/6 |

|(2) 106 " | 15 " | 1/7 |

|(3) 60 " | 8 " | 1/7 |

|(4) 80 " | 10 " | 1/8 |

+------------------------------------------------------------+

It will thus be seen that the upper side of the tendril is not totally

inexcitable, its power of contraction being about one-seventh that of

the under side.

NEGATIVE CURVATURE OF THE TENDRIL.

I shall now describe certain remarkable results which show that under

certain definite conditions the tendril moves away from the stimulated

side. I have explained, how in growing organs the effect of unilateral

stimulus longitudinally transmitted, induces an expansion higher up on

the same side to which the stimulus is applied, resulting in convexity

and movement away from the stimulus (cf. Laws of Tropic Curvatures, p.

286). As the reaction of tendril is in no way different from that of

growing organs in general, it occurred to me that it would be possible

to induce in it a negative curvature by application of indirect

unilateral stimulus.

_Experiment 110._--A tendril of _Passiflora_ was held in a clamp, as in

the diagram (Fig. 106) in which the left is the more excitable side of

the organ. The responsive movement of the tendril is observed by

focussing a reading microscope on a mark on the upper part of the

tendril. Direct mechanical stimulation at the dotted arrow makes the

tendril move in the same direction, the response being _positive_. But

if stimulus be applied on the same side below the clamp the tendril is

found to move away from stimulus, the response being now _negative_.

This reversal of response, as previously stated, is due to the fact that

the transmitted effect of indirect stimulus induces an acceleration of

growth higher up on the same side, which now becomes convex. The result

though unexpected, is in every way parallel to the response of the

flower bud of _Crinum_, in which the normal positive response was

converted into negative by changing the point of application of

stimulus, so that it became indirect (p. 216).

SUMMARY.

The response of tendril is in no way different from that of growing

organs in general.

Direct stimulus, electrical or mechanical, induces an incipient

contraction; the after-effect of a feeble stimulus is an acceleration of

growth above the normal. Indirect stimulus induces an enhancement of the

rate of growth.

Under unilateral mechanical stimulus of short duration the directly

excited proximal side undergoes contraction, the indirectly stimulated

distal side exhibits the opposite effect of expansion. The induced

curvature is thus due to the joint effects of the contraction of one

side, and the expansion of the opposite side.

As the after-effect of direct stimulus is an acceleration of growth

above the normal, the stimulated side undergoes an expansion by which

the recovery is hastened.

Unilateral application of direct stimulus induces a _positive_

curvature, but the same stimulus applied at a distance from the

responding region induces a _negative_ curvature.

The tendril of _Passiflora_ is excitable both on the upper and under

sides: the excitability of the under side is about seven times greater

than that of the upper side.

Stimulation of one side of the tendril induces an expansion of the

opposite side, even in cases where the contractility of the stimulated

side is feeble.

The response to stimulation of the more excitable side of the tendril is

thus inhibited by the stimulation of the opposite side. This is because

of the neutralisation of the effect of direct by that of indirect

stimulation.

XXVII.--ON GALVANOTROPISM

_By_

SIR J. C. BOSE,

_Assisted by_

GURUPRASANNA DAS.

Before describing the effect of unilateral application of an electrical

current in inducing tropic curvature, I shall give an account of the

polar effect of anode and cathode on the pulvinated and growing organs.

In my previous work[6] on the action of electrical current on sensitive

pulvini I have shown that:--

(1) at the 'make' of a current of moderate intensity a

contraction takes place at the cathode; the anode induces no

such contractile effect;

(2) at the 'make' of a stronger current both the anode and

cathode induce contraction.

[6] "Irritability of Plants," p. 212.

I have also carried out further investigations on the polar effect of

current on the autonomous activity of the leaflet of _Desmodium gyrans_.

These rhythmic pulsations can be recorded by my Oscillating Recorder.

Each pulsation consists of a sudden contractile movement downwards,

corresponding to the systole of a beating heart, and a slower up

movement of diastolic expansion. Application of cathode at the

pulvinule was found to exert a _contractile_ reaction, exhibited either

by the reduction of normal limit of diastolic expansion, or by an arrest

of movement at systole. The effect of anode was precisely the opposite;

the induced _expansion_ was exhibited either by reduction of normal

limit of systolic contraction, or by arrest of pulsation at diastole.

From the above results it is seen that with a feeble current:

(1) contraction is induced at the cathode, and

(2) expansion is brought about at the anode.

These effects take place under the action of a feeble current. Under

strong currents, contraction takes place both at the anode and the

cathode.

POLAR EFFECT OF ELECTRICAL CURRENT ON GROWTH.

The object of this investigation was to determine whether anode and

cathode exerted similar discriminative and opposite effects on growth.

For this experiment I took a specimen of _Kysoor_ and determined the

region where growth was maximum. A piece of moist cloth was wrapped

round this region to serve as one of the two electrodes. The second

electrode was placed in the neighbouring indifferent region where there

had been a cessation of growth.

_Effect of Cathode: Experiment 111._--The particular specimen of

_Kysoor_ had a normal rate of growth of 0·48 µ per second. On

application of the cathode the rate was reduced to 0·14 µ per second, or

to less than a third. This will be seen in record (Fig. 107), where N is

the normal rate of growth and K, retarded rate under the action of the

cathode.

[Illustration: FIG. 107.--Retardation of rate of growth under the action

of cathode (_Kysoor_).]

[Illustration: FIG. 108.--Acceleration of rate of growth under anode

(_Kysoor_).]

_Effect of anode: Experiment 112._--If the cathode induced a

retardation, the anode might be expected to induce an acceleration of

growth. But in my first experiment on the action of anode, I could

detect no perceptible variation of rate of growth. In trying to account

for this failure, I found that the specimen employed for the experiment

had normally a very rapid rate of growth. It appeared that an induced

acceleration would be brought out more conspicuously by choosing a

specimen in which the growth-rate was low, rather than in one in which

it was near its maximum. Acting on this idea, I took another specimen of

_Kysoor_ in which the normal rate was as slow as 0·10 µ per second. On

applying the anode to the growing region, there was an enhancement to

one and half times the normal rate (Fig. 108).

TABLE XXVIII.--EFFECT OF ANODE AND CATHODE ON GROWTH (_Kysoor_).

Specimen A Normal rate 0·10 µ per sec.

Acceleration under anode 0·155 µ per sec.

Specimen B Normal rate 0·48 µ per sec.

Retardation under cathode 0·14 µ per sec.

The effects given above take place under the action of a feeble current.

Strong current on the other hand induces a retardation or an arrest of

growth.

I have in the above experiments demonstrated the normal effect of anode

in inducing expansion and acceleration of rate of growth; the cathode

was shown to induce contraction and retardation of growth. Unilateral

application of anode and cathode thus induces appropriate curvatures in

pulvinated and in growing organs.

SUMMARY.

The effects of an electric current on growth is modified by the

direction of current. A feeble anodic current enhances the rate of

growth; a cathodic current on the other hand induces a retardation of

the rate. Strong current, both anodic and cathodic, induces a

retardation.

XXVIII.--ON THERMONASTIC PHENOMENA

_By_

SIR J. C. BOSE,

_Assisted by_

SURENDRA CHANDRA DAS.

In describing thermonastic curvatures Pfeffer says that "a special power

of thermonastic response has been developed by various flowers, in which

low temperatures produce closing movements, and high temperatures,

opening ones. The flowers of _Crocus vernus_ and _Crocus luteus_ are

specially responsive, as also those of _Tulipa Gesneriana_ for these

flowers perceptibly respond to a change of temperature of half a degree

centigrade."[7]

[7] Pfeffer--_Ibid_, Vol. III, p. 112.

We have hitherto studied the response of various organs to _stimulus_;

we have now to deal with the effect of thermal variation. Does rise of

temperature act like other forms of stimuli or is its action different?

We have therefore to find:

(1) The physiological effect of variation of temperature.

(2) Whether thermonastic irritability is confined only to

certain classes of organs, or is it a phenomenon of very wide

occurrence?

(3) Whether variation of temperature induces in anisotropic

organs only one type of response, or two types, positive and

negative.

(4) The law which determines the direction of responsive

movement.

EFFECT OF RISE OF TEMPERATURE.

As regards the effect of rise of temperature we have seen that, within

normal limits, it induces expansion and acceleration of the rate of

growth. Stimulus, on the other hand, induces precisely the opposite

effect. Hence the physiological reaction of steady rise of temperature

is, generally speaking, antagonistic to that of stimulus. This

conclusion is supported by numerous experiments which I have carried out

with various plant organs. Example of this will be found in the present

and subsequent chapters.

DIFFERENT THERMONASTIC ORGANS.

The only condition requisite for the exhibition of response is the

differential excitability of an anisotropic organ. It is therefore

likely to be exhibited by a large variety of plant organs, such as

pulvini, petioles, leaves, and flowers, and my results show that this is

actually the case. This particular sensibility, moreover, is not

confined to delicate structures, but is extended to rigid trees and

their branches.

Before proceeding further, it is necessary to draw attention to the

confusion which arises from the use of the common prefix '_thermo_' in

thermonasty and thermo-tropism. With regard to this Pfeffer says "It is

not known whether radiated and conducted heat exercise a similar

thermotropic reaction."[8] I shall show that the reactions to radiant

heat, and to conducted heat (rise of temperature) are of opposite

character, radiation inducing contraction, and rise of temperature,

expansion. It is therefore advisable to distinguish the thermal, or

temperature effect, from the radio-thermal effect of infra-red

radiation.

[8] Pfeffer--_Ibid_, Vol. III, p. 177.

TWO TYPES OF RESPONSE.

As regards the effect of variation of temperature I shall proceed to

show that there are two distinct types, which I shall, for convenience,

distinguish as the _Positive_ and _Negative_.

Positive thermonastic reaction is exhibited by organs in which the upper

half is the more excitable. Response to rise of temperature is by

_downward_ or _outward_ movement. In floral organs this finds expression

by a movement of opening. In illustration of this may be cited the

examples of the well known Crocus and also of _Zephyranthes_.

Negative thermonastic movement is shown by organs in which the lower

half is the more excitable. Here the response to rise of temperature is

by an _upward_ or _inward_ movement. I shall show that an example of

this is furnished by the flower of _Nymphæa_ which closes under rise,

and opens during fall of temperature.

POSITIVE THERMONASTIC RESPONSE.

_Response of Zephyranthes: Experiment 113._--Viewed from the top, the

inner side of the petal of a flower is the upper side. The _Crocus_

flower under rise of temperature opens outwards by expansion of the

inner side, which must be the more excitable. As _Crocus_ was not

available in Calcutta, I found the flower of _Zephyranthes_ (sometimes

called the Indian _Crocus_) reacting to variation of temperature in a

manner similar to that of _Crocus_, that is to say, the flower opens

under rise and closes with a fall of temperature. For obtaining record

all the perianth segments but one was removed. This segment was attached

to the recording lever. On lowering of temperature through 5°C. there

was an up-movement, or a movement of closure. Rise of temperature

induced, on the other hand, a movement of opening.

[Illustration: FIG. 109.--Thermonastic and radionastic responses of

petal of _Zephyranthes_ C, closing movement due to cooling, and H,

opening movement due to warming; R, closing movement due to

heat-radiation. Note opposite responses to rise of temperature and to

thermal radiation.]

_Effect of thermal radiation: Experiment 114._--I stated that the effect

of thermal radiation acts as a stimulus, inducing a reaction which is

antagonistic to that of rise of temperature. In verification of this, I

subjected the specimen to the action of infra-red radiation acting from

all sides. The result is seen in the responsive movement of closure

(Fig. 109 R). These experiments demonstrate clearly that the responses

to rise of temperature and thermal radiation are of opposite signs.

As a movement of closure was induced by the diffuse stimulus of thermal

radiation, it is evident that this must have been brought about by the

greater contraction of the inner half of the perianth; hence the inner

half of the organ is relatively the more excitable.

[Illustration: FIG. 110.--The Thermonastic Recorder. T, metallic

thermometer attached to the short arm of the upper lever; the specimen

of _Nymphæa_, N, has one of its perianth leaves attached to the short

arm of the second lever by a thread. C, clockwork for oscillation of the

plate.]

NEGATIVE THERMONASTIC RESPONSE.

_Response of_ Nymphæa: _Experiment 115._--Many of the Indian

_Nymphæaceæ_ have their sepals and petals closed during the day, and

open at night. I find that the perianth leaves of this flower are

markedly sensitive to variation of temperature. The Thermonastic

Recorder employed in this investigation is shown in figure 110. The

record given in figure 111 shows that the perianth segment, subjected to

a few degrees' rise of temperature, responded by an up-movement of

closure, due to greater expansion of the outer half. The latent period

was 6 seconds, and the maximum effect was attained in the further course

of 21 seconds. This experiment shows that the thermonastic response of

this flower is of the negative type.

[Illustration: FIG. 111.--Negative thermonastic response of _Nymphæa_.

Application of warmth at the vertical mark induced up-movement of

closure, but stimulus of electric shock at arrow induced rapid

excitatory down movement of opening. Successive dots at intervals of a

second.]

_Effect of stimulus: Experiment 116._--In the positive type of

thermonastic organs, where rise of temperature induced a movement of

opening, stimulus induced the opposite movement of closure (Expt. 114).

We shall now study the effect of stimulus on the movement of _Nymphæa_,

which undergoes closure during rise of temperature, as seen in the first

part of the record in figure 111. Stimulus of electric shock was applied

at the point marked with an arrow; the response is seen to be by a

movement of opening. Here also we find the effects of rise of

temperature and of stimulus to be antagonistic to each other. This will

be clearly seen in the following tabular statement.

TABLE XXIX.--SHOWING THE EFFECT OF RISE OF TEMPERATURE AND OF STIMULUS

ON THERMONASTIC ORGANS.

+---------------------------------------------------------------+

| Specimen. | Effect of rise | Effect of stimulus. |

| | of temperature. | |

+------------------+---------------------+----------------------+

| _Zephyranthes_ | Movement of opening | Movement of closure. |

| (positive type). | | |

| | | |

| _Nymphæa_ | Movement of closure | Movement of opening. |

| (negative type). | | |

+---------------------------------------------------------------+

In _Nymphæa_ it is the outer side of the perianth that is relatively the

more excitable since diffuse electric stimulus induces a movement of

opening due to the greater contraction of the outer side. It is by the

greater expansion of this more excitable side that the movement of

closure is effected during rise of temperature.

From the results of experiments given above we arrive at the

following:--

LAW OF THERMONASTIC REACTION

RISE OF TEMPERATURE INDUCES A GREATER EXPANSION OF THE MORE EXCITABLE

HALF OF AN ANISOTROPIC ORGAN.

SUMMARY.

Thermonastic movements are induced by the differential physiological

effect of variation of temperature on the two halves of an anisotropic

organ.

Rise of temperature induces greater expansion, and enhancement of rate

of growth of the more excitable half of the organ; lowering of

temperature induces the opposite effect.

Two types of thermonastic movements are met with, the _positive_

exhibiting a movement of opening during rise of temperature; in these

the inner half of the organ is relatively the more excitable. Example of

this is seen in the _Crocus_ and in _Zephyranthes_.

In the _negative_ type, rise of temperature induces a movement of

closure. Here the outer half of the organ is the more excitable. The

flower of _Nymphæa_ belongs to this type.

The effect of stimulus is antagonistic to that of rise of temperature.

In positive thermonastic organs stimulus induces a movement of closure;

in the negative type it induces a movement of opening.

XXIX.--ON PHOTOTROPISM

_By_

SIR J. C. BOSE.

In different organs of plants the stimulus of light induces movements of

an extremely varied character. Radial organs exhibit tropic movements in

which the position of equilibrium is definitely related to the direction

of incident stimulus. Nastic movements under the action of light are, on

the other hand, regarded as curvatures of the organ which show "no

relation to the stimulus but is determined by the activity of the plant

itself".[9] There are thus two classes of response to light which seem

to be unrelated to each other. Returning to the directive action of

light, radial stems often bend towards the light, while certain roots

bend away from it. It may be thought that this difference is due to

specific difference of irritability between shoot and root, the

irritability of the former being of a positive, and of the latter, of a

negative character. But there are numerous exceptions to this

generalisation. Certain roots bend towards the light, while a stem,

under different circumstances, moves towards light or away from it.

Again an identical organ may exhibit a positive or a negative curvature.

Thus the leaflets of _Mimosa pudica_ acted on by light from above fold

upwards, the phototropic effect being _positive_. But the same leaflets

acted on by light from below exhibit a folding upwards, the phototropic

effect being now _negative_. Effects precisely the opposite are found

with the leaflets of _Biophytum_ and _Averrhoa_. They fold downwards

whether light acts from above or below. Finally, a radial organ in

found to exhibit under light of increasing intensity or duration, a

positive, a dia-phototropic, or a negative phototropic curvature.

[9] Jost--_Ibid_, p. 428.

In these circumstances the theory of specific positive and negative

irritabilities is untenable; in any case, it throws no light on the

phenomenon of movement. The difficulties of the problem are thus clearly

stated by Pfeffer: "When we say that an organ curves towards a source of

illumination, because of its heliotropic irritability and we are simply

expressing an ascertained fact in a conveniently abbreviated form,

without explaining why such curvature is possible or how it is

produced.... Many observers have unfortunately devoted their attention

to artificially classifying the phenomenon observed, and have entirely

neglected the explanation of causes underlying them."[10]

[10] Pfeffer--_Ibid_, Vol. II, p. 74.

COMPLEXITY OF PROBLEM OF PHOTOTROPIC REACTION.

The complexity of phototropic reaction arises from the summated effects

of numerous factors; for explanation of the resultant response it is

therefore necessary to take full account of the individual effect of

each of them.

Among these operative factors in phototropic reaction may be

mentioned:--

(1) The difference of effects induced by light at the proximal

and distal sides of the organ.

(2) The modification of the latent period with the intensity of

stimulus.

(3) The after-effect of stimulus.

(4) The modifying influence of tonic condition on response.

(5) The effect of direction of light.

(6) The effect of intensity of light.

(7) The effect of duration of stimulation.

(8) The transmitted effect of light.

(9) The effect of unequal excitability in different zones of

the organ.

(10) The effect of transverse conduction in modification of

the sign of response.

(11) The effect of temperature on phototropic action.

(12) The modification of response due to differential

excitability of the organ.

(13) Nastic and tropic reactions.

(14) The torsional effect of light.

The sketch given above will give us some idea of the complexity of the

problem. In this and in the following papers I shall describe the

investigations I have carried out on the subjects detailed above.

ACTION OF LIGHT.

I have shown that there is no essential difference between the responses

of pulvinated and growing organs, that diminution of turgor induced by

stimulus brings about contraction in the one, and retardation of the

rate of growth in the other. Indirect stimulation, on the other hand,

induces an expansion and acceleration of the rate of growth. The

experimental investigation on the tropic effect of light may therefore

be carried out both with pulvinated and growing organs.

As regards the effect of direct stimulus of light on growing organs we

found (p. 208) that it induces an incipient contraction, seen in

diminution of the rate of growth; this incipient contraction culminates

in an actual contraction under increasing intensity of light. The

contraction under direct stimulation is also observed in pulvinated

organs. When light acts from above the upper half of the pulvinus

undergoes contraction, resulting in erection of the motile leaf or

leaflets. As regards the effect of indirect unilateral stimulus of light

on the distal side of the organ, we found that its effect is an

enhancement of turgor (p. 281). Hence the positive tropic curvature

under light is brought about, as in the case of other forms of stimuli,

by the contraction of the proximal, and expansion of the distal sides of

the organ.

Various analogies have been noticed between phototropic and geotropic

reactions, and it has been supposed that the two phenomena are closely

related to each other. This has even led to assumption that there are

phototropic particles which function like statoliths in geotropic

organs. There is, however, certain outstanding difference between the

two classes of phenomena. In the case of light, the incident energy is

entirely derived from the outside. But in geotropism, the force of

gravity by itself is ineffective without the intervention of the weight

of cell-contents to exert pressure on the sensitive ectoplasm, and thus

induce stimulation. This aspect of the subject will be treated in

greater detail in a subsequent chapter.

POSITIVE PHOTOTROPIC CURVATURE.

I shall now describe the phototropic effect of unilateral light in

pulvinated, and in growing organs. From the explanation that has already

been given, it will be understood that the side of the organ directly

acted on by light undergoes contraction and concavity.

_Tropic curvature of pulvinated organs: Experiment 117._--For this

experiment I employed the terminal leaflet of the bean plant. The

source of illumination was 32 c.p. electric lamp, enclosed in a metallic

tube with circular aperture for passage of light. The leaflet was

attached to an Oscillating Recorder. Light was applied on the upper half

of the pulvinus for 20 seconds; this induced an up-movement of the

leaflet, due to the contraction of the upper half of the organ. Recovery

took place in course of 8 minutes (Fig. 112).

[Illustration: FIG. 112.--Successive positive responses of the terminal

leaflet of bean. Light applied from above for 20 seconds; complete

recovery in 8 minutes.]

POSITIVE PHOTOTROPIC CURVATURE OF GROWING ORGANS.

_Effect of moderate stimulation: Experiment 118._--I shall presently

show that the intensity of phototropic reaction depends on the

intensity and duration of the incident light. A moderate and effective

stimulation may thus be produced by short exposure to strong light. For

my present experiment I took a stem of _Dregea volubilis_, and applied

light from a small arc lamp to one side of the organ for 1 minute; this

induced a positive curvature followed by complete recovery on the

cessation of light (Fig. 113).

[Illustration: FIG. 113.--Positive curvature under moderate phototropic

stimulation. Note complete recovery (_Dregea_).]

[Illustration: FIG. 114.--Persistent positive curvature under stronger

stimulation (_Dregea_).]

_Effect of strong stimulation: Experiment 119._--After recovery of the

stem of the last experiment, the same light was applied for 5 minutes.

It is seen that the curvature is greatly increased (Fig. 114). Thus the

phototropic curvature increases, within limits, with the duration of

stimulation. The curvature induced under stronger stimulation remained

more or less persistent. In certain instances there was a partial

recovery after a considerable length of time; in others curvature was

fixed by growth.

PHENOMENON OF RECOVERY.

On the cessation of stimulus of moderate intensity the heliotropically

curved organ straightens itself; similar effects are also found in other

tropic curvatures. Thus a tendril straightens itself after curvature

induced by contact of short duration. The theory of rectipitality has

been proposed to account for the recovery, which assumes the action of

an unknown regulating power by which the organ is brought back to a

straight line; but beyond the assumption of an unknown specific power,

the theory affords no explanation of the mechanism by which this is

brought about.

The problem before us is to find out the means by which the organ

straightens itself after brief stimulation. It will also be necessary to

find out why there is no recovery after prolonged stimulation. We have

thus to investigate the after-effect of stimulus of various intensities

on growth, and the Balanced Method of recording Growth offers us an

unique opportunity of studying the characteristic after-effects.

IMMEDIATE AND AFTER-EFFECT OF LIGHT ON GROWTH.

As regards the effect of light I have already shown:

(1) that a sub-minimal stimulus induces an acceleration of

growth, but under long continued action the acceleration is

converted into normal retardation (p. 225),

(2) that a stimulus of moderate intensity induces the normal

retardation of the rate of growth.

It is evident that there is a _critical intensity_ of stimulus, above

which there is a retardation, and below which there is the opposite

reaction of acceleration. This critical intensity, I have found to be

low in vigorous specimens, and high in sub-tonic specimens. Thus the

same intensity of stimulus may induce a retardation of growth in

specimens the tonic condition of which is _above par_, and an

acceleration in others, in which it is _below par_. The following

experiments will demonstrate the immediate and after-effect of light of

increasing intensity and duration.

[Illustration: FIG. 115.--Immediate and after-effect of stimulus of

light on growth. (_a_) shows immediate effect of moderate light to be a

transitory acceleration (down-curve) followed by retardation (up-curve).

The after-effect on cessation of light is an acceleration (down-curve)

followed by restoration to normal. (_b_) Immediate and after-effect of

stronger light: immediate effect, a retardation; after-effect, recovery

to normal rate without acceleration.]

_Effect of light of moderate intensity: Experiment 120._--The source of

light was a small arc lamp placed at a distance of 50 cm., the intensity

of incident light was increased or decreased by bringing the source of

light nearer or further away from the plant. Two inclined mirrors were

placed behind the plant so that the specimen was acted on by light from

all sides. A seedling of wheat was mounted on the Balanced Crescograph,

and record was first taken under exact balance; this gives a horizontal

record. The up-curve represents retardation, and down-curve acceleration

of rate of growth. The source of light was at first placed at a distance

of 50 cm. from the plant, and exposure was given for 4 minutes at the

point marked with an arrow (Fig. 115a). We shall find in the next

chapter that the _intensity of phototropic effect is proportional to the

quantity of incident light_. This quantity at the beginning proved to be

sub-minimal, and hence there was an acceleration at the beginning.

Continued action induced the normal effect of retardation, as seen in

the subsequent resulting up-curve. On the cessation of light, the

balance was upset in an opposite direction, the resulting down-curve

showing an acceleration of the rate of growth above the normal. This

acceleration persisted for a time, after which the normal rate of growth

was restored, as seen in the curve becoming once more horizontal. _The

after-effect of light of moderate intensity is thus a temporary

acceleration of rate of growth above the normal._

_Effect of strong light: Experiment 121._--The same specimen was used as

in the last experiment. By bringing the source of light to a distance of

25 cm. the intensity of light was increased fourfold; the duration of

exposure was kept the same as before. The record (Fig. 115b) shows that

a retardation of rate of growth occurred from the very beginning without

the preliminary acceleration. This is for two reasons: (1) the increased

intensity was now above the critical minimum, and (2) the tone of the

organ had become improved by previous stimulation. On the cessation of

light, the after-effect showed no enhancement of rate of growth, the

recovery from retardation to the normal rate being gradual. In the next

experiment (the result of which is not given in the record) the

intensity of light was increased still further; the retardation now

became very marked, and it persisted for a long time even on the

cessation of light.

We thus find that:

(1) The immediate effect of light of moderate intensity is a

preliminary acceleration, followed by normal retardation. The

acceleration is the effect of sub-minimal stimulation. The

immediate after-effect is an acceleration above the normal.

(2) The immediate effect of strong light is a retardation

from the beginning; the immediate after-effect shows no

acceleration, the growth rate being gradually restored to the

normal.

(3) Under very strong light the induced retardation is very

great, and this persists for a long time even on the removal

of light.

Life Movements in Plants, Volume II · 第 3 / 7 章