By comparing the flipper of the seal, sea-bear, and walrus with the

fin and tail of the fish, whale, porpoise, etc.; and the wing of the

penguin (a bird which is incapable of flight, and can only swim and

dive) with the wing of the insect, bat, and bird, I have been able

to show that a close analogy exists between the flippers, fins, and

tails of sea mammals and fishes on the one hand, and the wings of

insects, bats, and birds on the other; in fact, that theoretically and

practically these organs, one and all, form flexible helices or screws,

which, in virtue of their rapid reciprocating movements, operate upon

the water and air by a wedge-action after the manner of twisted or

double inclined planes. The twisted inclined planes act upon the air

and water by means of curved surfaces, the curved surfaces reversing,

reciprocating, and engendering a wave pressure, which can be continued

indefinitely at the will of the animal. The wave pressure emanates in

the one instance mainly from the tail of the fish, whale, porpoise,

etc., and in the other from the wing of the insect, bat, or bird--_the

reciprocating and opposite curves_ into which the tail and wing are

thrown in swimming and flying constituting _the mobile helices, or

screws_, which, during their action, produce the precise kind and

degree of pressure adapted to fluid media, and to which they respond

with the greatest readiness.

In order to prove that sea mammals and fishes swim, and insects, bats,

and birds fly, by the aid of curved figure-of-8 surfaces, which exert

an intermittent wave pressure, I constructed artificial fish-tails,

fins, flippers, and wings, which curve and taper in every direction,

and which are flexible and elastic, particularly towards the tips

and posterior margins. These artificial fish-tails, fins, flippers,

and wings are slightly twisted upon themselves, and when applied to

the water and air by a sculling or figure-of-8 motion, curiously

enough reproduce the curved surfaces and movements peculiar to real

fish-tails, fins, flippers, and wings, in swimming, and flying.

Propellers formed on the fish-tail and wing model are, I find, the

most effective that can be devised, whether for navigating the water

or the air. To operate efficiently on fluid, _i.e._ yielding media,

the propeller itself must yield. Of this I am fully satisfied from

observation and experiment. The propellers at present employed in

navigation are, in my opinion, faulty both in principle and application.

The observations and experiments recorded in the present volume date

from 1864. In 1867 I lectured on the subject of animal mechanics at

the Royal Institution of Great Britain:[7] in June of the same year

(1867) I read a memoir “On the Mechanism of Flight” to the Linnean

Society of London;[8] and in August of 1870 I communicated a memoir “On

the Physiology of Wings” to the Royal Society of Edinburgh.[9] These

memoirs extend to 200 pages quarto, and are illustrated by 190 original

drawings. The conclusions at which I arrived, after a careful study of

the movements of walking, swimming, and flying, are briefly set forth

in a letter addressed to the French Academy of Sciences in March 1870.

This the Academy did me the honour of publishing in April of that year

(1870) in the Comptes Rendus, p. 875. In it I claim to have been the

first to describe and illustrate the following points, viz.:--

[7] “On the various modes of Flight in relation to

Aëronautics.”--Proceedings of the Royal Institution of Great Britain,

March 22, 1867.

[8] “On the Mechanical Appliances by which Flight is attained in the

Animal Kingdom.”--Transactions of the Linnean Society, vol. xxvi.

[9] “On the Physiology of Wings.”--Transactions of the Royal Society

of Edinburgh, vol. xxvi.

That quadrupeds walk, and fishes swim, and insects, bats, and birds fly

by figure-of-8 movements.

That the flipper of the sea bear, the swimming wing of the penguin, and

the wing of the insect, bat, and bird, are screws _structurally_, and

resemble the blade of an ordinary screw-propeller.

That those organs are screws _functionally_, from their twisting and

untwisting, and from their rotating in the direction of their length,

when they are made to oscillate.

That they have a reciprocating action, and reverse their planes more or

less completely at every stroke.

That the wing describes _a figure-of-8 track_ in space when the flying

animal is artificially fixed.

That the wing, when the flying animal is progressing at a high speed

in a horizontal direction, describes _a looped_ and then _a waved

track_, from the fact that the figure of 8 is gradually opened out or

unravelled as the animal advances.

That the wing acts after the manner of a kite, both during the down and

up strokes.

I was induced to address the above to the French Academy from finding

that, nearly two years after I had published my views on the figure

of 8, looped and wave movements made by the wing, etc., Professor

E. J. Marey (College of France, Paris) published a course of lectures,

in which the peculiar figure-of-8 movements, first described and

figured by me, were put forth as a new discovery. The accuracy of this

statement will be abundantly evident when I mention that my first

lecture, “On the various modes of Flight in relation to Aëronautics,”

was published in the Proceedings of the Royal Institution of Great

Britain on the 22d of March 1867, and translated into French (Revue

des cours scientifiques de la France et de l’Étranger) on the 21st

of September 1867; whereas Professor Marey’s first lecture, “On the

Movements of the Wing in the Insect” (Revue des cours scientifiques de

la France et de l’Étranger), did not appear until the 13th of February

1869.

Professor Marey, in a letter addressed to the French Academy in reply

to mine, admits my claim to priority in the following terms:--

“J’ai constaté qu’effectivement M. Pettigrew a vu avant moi, et

représenté dans son Mémoire, la forme en 8 du parcours de l’aile de

l’insecte: que la méthode optique à laquelle j’avais recours est à peu

près identique à la sienne.... Je m’empresse de satisfaire à cette

demande légitime, et de laisser entièrement la priorité sur moi à M.

Pettigrew relativement à la question ainsi restreinte.”--(Comptes

Rendus, May 16, 1870, p. 1093).

The figure-of-8 theory of walking, swimming, and flying, as originally

propounded in the lectures, papers, and memoirs referred to, has been

confirmed not only by the researches and experiments of Professor

Marey, but also by those of M. Senecal, M. de Fastes, M. Ciotti, and

others. Its accuracy is no longer a matter of doubt. As the limits

of the present volume will not admit of my going into the several

arrangements by which locomotion is attained in the animal kingdom as

a whole, I will only describe those movements which illustrate in a

progressive manner the several kinds of progression on the land, and on

and in the water and air.

I propose first to analyse the natural movements of walking, swimming,

and flying, after which I hope to be able to show that certain of these

movements may be reproduced artificially. The locomotion of animals

depends upon mechanical adaptations found in all animals which change

locality. These adaptations are very various, but under whatever guise

they appear they are substantially those to which we resort when we

wish to move bodies artificially. Thus in animal mechanics we have

to consider the various orders of levers, the pulley, the centre of

gravity, specific gravity, the resistance of solids, semi-solids,

fluids, etc. As the laws which regulate the locomotion of animals are

essentially those which regulate the motion of bodies in general, it

will be necessary to consider briefly at this stage the properties of

matter when at rest and when moving. They are well stated by Mr. Bishop

in a series of propositions which I take the liberty of transcribing:--

“_Fundamental Axioms._--First, every body continues in a state of rest,

or of uniform motion in a right line, until a change is effected by

the agency of some mechanical force. Secondly, any change effected in

the quiescence or motion of a body is in the direction of the force

impressed, and is proportional to it in quantity. Thirdly, reaction

is always equal and contrary to action, or the mutual actions of two

bodies upon each other are always equal and in opposite directions.

“_Of uniform motion._--If a body moves constantly in the same manner,

or if it passes over equal spaces in equal periods of time, its motion

is uniform. The velocity of a body moving uniformly is measured by the

space through which it passes in a given time.

“The velocities generated or impressed on different masses by the same

force are reciprocally as the masses.

“_Motion uniformly varied._--When the motion of a body is uniformly

accelerated, the space it passes through during any time whatever is

proportional to the square of the time.

“In the leaping, jumping, or springing of animals in any direction

(except the vertical), the paths they describe in their transit from

one point to another in the plane of motion are parabolic curves.

“_The legs move by the force of gravity as a pendulum._--The Professor,

Weber, have ascertained, that when the legs of animals swing forward in

progressive motion, they obey the same laws as those which regulate the

periodic oscillations of the pendulum.

“_Resistance of fluids._--Animals moving in air and water experience

in those media a sensible resistance, which is greater or less in

proportion to the density and tenacity of the fluid, and the figure,

superficies, and velocity of the animal.

“An inquiry into the amount and nature of the resistance of air and

water to the progression of animals will also furnish the data for

estimating the proportional values of those fluids acting as fulcra to

their locomotive organs, whether they be fins, wings, or other forms of

lever.

“The motions of air and water, and their directions, exercise very

important influences over velocity resulting from muscular action.

“_Mechanical effects of fluids on animals immersed in them._--When a

body is immersed in any fluid whatever, it will lose as much of its

weight relatively as is equal to the weight of the fluid it displaces.

In order to ascertain whether an animal will sink or swim, or be

sustained without the aid of muscular force, or to estimate the amount

of force required that the animal may either sink or float in water, or

fly in the air, it will be necessary to have recourse to the specific

gravities both of the animal and of the fluid in which it is placed.

“The specific gravities or comparative weights of different substances

are the respective weights of equal volumes of those substances.

“_Centre of gravity._--The centre of gravity of any body is a

point about which, if acted upon only by the force of gravity, it

will balance itself in all positions; or, it is a point which, if

supported, the body will be supported, however it may be situated in

other respects; and hence the effects produced by or upon any body

are the same as if its whole mass were collected into its centre of

gravity.

“The attitudes and motions of every animal are regulated by the

positions of their centres of gravity, which, in a state of rest, and

not acted upon by extraneous forces, must lie in vertical lines which

pass through their basis of support.

“In most animals moving on solids, the centre is supported by variously

adapted organs; during the flight of birds and insects it is suspended;

but in fishes, which move in a fluid whose density is nearly equal

to their specific gravity, the centre is acted upon equally in all

directions.”[10]

[10] Cyc. of Anat. and Phy., Art. “Motion,” by John Bishop, Esq.

As the locomotion of the higher animals, to which my remarks more

particularly apply, is in all cases effected by levers which differ in

no respect from those employed in the arts, it may be useful to allude

to them in a passing way. This done, I will consider the bones and

joints of the skeleton which form the levers, and the muscles which

move them.

“_The Lever._--Levers are commonly divided into three kinds, according

to the relative positions of the prop or fulcrum, the power, and the

resistance or weight. The straight lever of each order is equally

balanced when the power multiplied by its distance from the fulcrum

equals the weight, multiplied by its distance, or P the power, and

W the weight, are in equilibrium when they are to each other in the

inverse ratio of the arms of the lever, to which they are attached. The

pressure on the fulcrum however varies.

[Illustration: FIG. 1.]

“In straight levers of the _first kind_, the fulcrum is between the

power and the resistance, as in fig. 1, where F is the fulcrum of the

lever AB; P is the power, and W the weight or resistance. We have

P : W :: BF : AF, hence P.AF = W.BF, and the pressure on the fulcrum is both

the power and resistance, or P + W.

“In the second order of levers (fig. 2), the resistance is between

the fulcrum and the power; and, as before, P : W :: BF : AF, but the

pressure of the fulcrum is equal to W - P, or the weight less the power.

[Illustration: FIG. 2.]

“In the third order of lever the power acts between the prop and the

resistance (fig. 3), where also P : W :: BF : AF, and the pressure on

the fulcrum is P - W, or the power less the weight.

[Illustration: FIG. 3.]

“In the preceding computations the weight of the lever itself is

neglected for the sake of simplicity, but it obviously forms a part of

the elements under consideration, especially with reference to the arms

and legs of animals.

“To include the weight of the lever we have the following equations:

P.AF + {AF}.1/2AF = W.BF + {BF}.1/2BF; in the first order, where

{AF} and {BF} represent the weights of these portions of the lever

respectively. Similarly, in the second order P.AF = W.BF + {AF}.(AF)/2,

and in the third order P.AF = W.BF + {BF}.(BF)/2.

“In this outline of the theory of the lever, the forces have been

considered as acting vertically, or parallel to the direction of the

force of gravity.

“_Passive Organs of Locomotion. Bones._--The solid framework or

skeleton of animals which supports and protects their more delicate

tissues, whether chemically composed of entomoline, carbonate, or

phosphate of lime; whether placed internally or externally; or whatever

may be its form or dimensions, presents levers and fulcra for the

action of the muscular system, in all animals furnished with earthy

solids for their support, and possessing locomotive power.”[11] The

levers and fulcra are well seen in the extremities of the deer, the

skeleton of which is selected for its extreme elegance.

[11] Bishop, _op. cit._

[Illustration:

FIG. 4. Skeleton of the Deer (after Pander and D’Alton). The bones

in the extremities of this the fleetest of quadrupeds are inclined

very obliquely towards each other, and towards the scapular and

iliac bones. This arrangement increases the leverage of the muscular

system and confers great rapidity on the moving parts. It augments

elasticity, diminishes shock, and indirectly begets continuity of

movement, _a._ Angle formed by the femur with the ilium, _b._ Angle

formed by the tibia and fibula with the femur, _c._ Angle formed by

the cannon bone with the tibia and fibula, _d._ Angle formed by the

phalanges with the cannon bone. _e._ Angle formed by the humerus

with the scapula. _f._ Angle formed by the radius and ulna with the

humerus.]

While the bones of animals form levers and fulcra for portions of the

muscular system, it must never be forgotten that the earth, water, or

air form fulcra for the travelling surfaces of animals as a whole.

Two sets of fulcra are therefore always to be considered, viz. those

represented by the bones, and those represented by the earth, water,

or air respectively. The former when acted upon by the muscles produce

motion in different parts of the animal (not necessarily progressive

motion); the latter when similarly influenced produce locomotion.

Locomotion is greatly favoured by the tendency which the body once

set in motion has to advance in a straight line. “The form, strength,

density, and elasticity of the skeleton varies in relation to the bulk

and locomotive power of the animal, and to the media in which it is

destined to move.

“The number of moveable articulations in a skeleton determines the

degree of its mobility within itself; and the kind and number of

the articulations of the locomotive organs determine the number and

disposition of the muscles acting upon them.

“The bones of vertebrated animals, especially those which are

entirely terrestrial, are much more elastic, hard, and calculated by

their chemical elements to bear the shocks and strains incident to

terrestrial progression, than those of the aquatic vertebrata; the

bones of the latter being more fibrous and spongy in their texture, the

skeleton is more soft and yielding.

“The bones of the higher orders of animals are constructed according

to the most approved mechanical principles. Thus they are convex

externally, concave within, and strengthened by ridges running across

their discs, as in the scapular and iliac bones; an arrangement which

affords large surfaces for the attachment of the powerful muscles of

locomotion. The bones of birds in many cases are not filled with marrow

but with air,--a circumstance which insures that they shall be very

strong and very light.

“In the thigh bones of most animals an angle is formed by the head

and neck of the bone with the axis of the body, which prevents the

weight of the superstructure coming vertically upon the shaft, converts

the bone into an elastic arch, and renders it capable of supporting

the weight of the body in standing, leaping, and in falling from

considerable altitudes.

“_Joints._--Where the limbs are designed to move to and fro simply

in one plane, the ginglymoid or hinge-joint is applied; and where

more extensive motions of the limbs are requisite, the enarthrodial,

or ball-and-socket joint, is introduced. These two kinds of joints

predominate in the locomotive organs of the animal kingdom.

“The enarthrodial joint has by far the most extensive power of

motion, and is therefore selected for uniting the limbs to the trunk.

It permits of the several motions of the limbs termed pronation,

supination, flexion, extension, abduction, adduction, and revolution

upon the axis of the limb or bone about a conical area, whose apex is

the axis of the head of the bone, and base circumscribed by the distal

extremity of the limb.”[12]

[12] Bishop, _op. cit._

The ginglymoid or hinge-joints are for the most part spiral in their

nature. They admit in certain cases of a limited degree of lateral

rocking. Much attention has been paid to the subject of joints

(particularly human ones) by the brothers Weber, Professor Meyer

of Zürich, and likewise by Langer, Henke, Meissner, and Goodsir.

Langer, Henke, and Meissner succeeded in demonstrating the “screw

configuration” of the articular surfaces of the elbow, ankle, and

calcaneo-astragaloid joints, and Goodsir showed that the articular

surface of the knee-joint consist of “a double conical screw

combination.” The last-named observer also expressed his belief “that

articular combinations with opposite windings on opposite sides of

the body, similar to those in the knee-joint, exist in the ankle and

tarsal, and in the elbow and carpal joints; and that the hip and

shoulder joints consist of single threaded couples, but also with

opposite windings on opposite sides of the body.” I have succeeded

in demonstrating a similar spiral configuration in the several bones

and joints of the wing of the bat and bird, and in the extremities of

most quadrupeds. The bones of animals, particularly the extremities,

are, as a rule, twisted levers, and act after the manner of screws.

This arrangement enables the higher animals to apply their travelling

surfaces to the media on which they are destined to operate at any

degree of obliquity so as to obtain a maximum of support or propulsion

with a minimum of slip. If the travelling surfaces of animals did not

form screws structurally and functionally, they could neither seize

nor let go the fulcra on which they act with the requisite rapidity to

secure speed, particularly in water and air.

“_Ligaments._--The office of the ligaments with respect to locomotion,

is to restrict the degree of flexion, extension, and other motions of

the limbs within definite limits.

“_Effect of Atmospheric pressure on Limbs._--The influence of

atmospheric pressure in supporting the limbs was first noticed by Dr.

Arnott, though it has been erroneously ascribed by Professor Müller

to Weber. Subsequent experiments made by Dr. Todd, Mr. Wormald, and

others, have fully established the mechanical influence of the air in

keeping the mechanism of the joints together. The amount of atmospheric

pressure on any joint depends upon the area or surface presented to its

influence, and the height of the barometer. According to Weber, the

atmospheric pressure on the hip-joint of a man is about 26 lbs. The

pressure on the knee-joint is estimated by Dr. Arnott at 60 lbs.”[13]

[13] Bishop, _op. cit._

[Illustration:

FIG. 5. Shows the muscular cycle formed by the biceps (_a_) or flexor

muscle, and the triceps (_b_) or extensor muscle of the human arm. At

_i_ the centripetal or shortening action of the biceps is seen, and

at _j_ the centrifugal or elongating action of the triceps (_vide_

arrows). The present figure represents the forearm as flexed upon

the arm. As a consequence, the long axes of the sarcous elements or

ultimate particles of the biceps (_i_) are arranged in a more or less

horizontal direction; the long axes of the sarcous elements of the

triceps (_j_) being arranged in a nearly vertical direction. When

the forearm is extended, the long axes of the sarcous elements of

the biceps and triceps are reversed. The present figure shows how

the bones of the extremities form levers, and how they are moved

by muscular action. If, _e.g._, the biceps (_a_) shortens and the

triceps (_b_) elongates, they cause the forearm and hand (_h_) to

move towards the shoulder (_d_). If, on the other hand, the triceps

(_b_) shortens and the biceps (_a_) elongates, they cause the forearm

and hand (_h_) to move away from the shoulder. In these actions the

biceps (_a_) and triceps (_b_) are the power; the elbow-joint (_g_)

the fulcrum, and the forearm and hand (_h_) the weight to be elevated

or depressed. If the hand represented a travelling surface which

operated on the earth, the water, or the air, it is not difficult to

understand how, when it was made to move by the action of the muscles

of the arm, it would in turn move the body to which it belonged, _d_

Coracoid process of the scapula, from which the internal or short

head of the biceps (_a_) arises, _e_ Insertion of the biceps into

the radius. _f_ Long head of the triceps (_b_). _g_ Insertion of the

triceps into the olecranon process of the ulna.--_Original._]

Animal Locomotion; or, walking, swimming, and flying With a dissertation on aëronautics · 第 2 / 23 段