Towards the close of the day the atmosphere became very serene. A few

distant cumuli sailed near the horizon, but the zenith and a vast

angular space all round it were absolutely free from cloud. From the

deck of the 'Galatea' a rocket was discharged, which reached a great

elevation, and exploded with a loud report. Following this solid

nucleus of sound was a continuous train of echoes, which retreated to

a continually greater distance, dying gradually off into silence after

seven seconds' duration. These echoes were of the same character as

those so frequently noticed at the South Foreland in 1872-73, and

called by me 'aerial echoes.'

On the 23rd of March the experiments were resumed, the most noteworthy

results of that day's observations being that the sounds were heard at

Tillingham, 10 miles to the N.E.; at West Mersea, 15.75 miles to the

N.E. by E; at Brightlingsea, 17.5 miles to the N.E.; and at Clacton

Wash, 20.5 miles to the N.E. by 1/2 E. The wind was blowing at the

time from the S.E. Some of these sounds were produced by rockets,

some by a 24-lb. howitzer, and some by an 8-inch Maroon.

In December, 1876, Mr. Gardiner, the managing director of the

Cotton-powder Company, had proposed a trial of this material against

the gun-cotton. The density of the cotton he urged was only 1.03,

while that of the powder was 1.70. A greater quantity of explosive

material being thus compressed into the same volume, Mr. Gardiner

thought that a greater sonorous effect must be produced by the powder.

At the instance of Mr. Mackie, who had previously gone very

thoroughly into the subject, a Committee of the Elder Brethren visited

the cotton-powder manufactory, on the banks of the Swale, near

Faversham, on the 16th of June, 1877. The weights of cotton-powder

employed were 2 oz, 8 oz, 1 lb, and 2 lbs, in the form of rockets and

of signals fired a few feet above the ground. The experiments

throughout were arranged and conducted by Mr. Mackie. Our desire on

this occasion was to get 'as near to windward as possible, but the

Swale and other obstacles limited our distance to 1.5 mile. We stood

here E.S.E. from the firing-point while the wind blew fresh from the

N.E.

The cotton-powder yielded a very effective report. The rockets in

general had a slight advantage over the same quantities of material

fired near the ground. The loudness of the sound was by no means

proportional to the quantity of the material exploded, 8 oz. yielding

very nearly as loud a report as 1 lb. The 'aerial echoes,' which

invariably followed the explosion of the rockets, were loud and

long-continued.

On the 17th of October, 1877, another series of experiments with

howitzers and rockets was carried out at Shoeburyness. The charge of

the howitzer was 3 lbs. of L. G. powder. The charges of the rockets

were 12 oz, 8 oz, 4 oz, and 2 oz. of gun-cotton respectively. The gun

and the four rockets constituted a series, and eight series were fired

during the afternoon of the 17th. The observations were made from the

'Vestal' and the 'Galatea,' positions being successively assumed which

permitted the sound to reach the observers with the Wind, against the

wind, and across the wind. The distance of the 'Galatea' varied from

3 to 7 miles, that of the 'Vestal,' which was more restricted in her

movements, being 2 to 3 miles. Briefly summed up, the result is that

the howitzer, firing a 3-lb. charge, which it will be remembered was

our best gun at 'the South Foreland, was beaten by the 12-oz. rocket,

by the 8-oz. rocket, and by the 4-oz. rocket. The 2-oz. rocket alone

fell behind the howitzer.

It is worth while recording the distances at which some of the sounds

were heard on the day now referred to:

1. Leigh 6.5 miles W.N.W. 24 out of 40 sounds heard.

2. Girdler 12 miles S.E. by E. 5 out of 40 sounds heard.

Light-vessel

3. Reculvers 171 miles S.E. by S. 18 out of 40 sounds heard.

4. St. Nicholas 20 miles S.E. 3 out of 40 sounds heard.

5. Epple Bay 22 miles S.E. by E. 19 out of 40 sounds heard.

6. Westgate 23 miles S.E. by E. 9 out of 40 sounds heard.

7. Kingsgate 25 miles S.E. by E. 8 out of 40 sounds heard.

The day was cloudy, with occasional showers of drizzling rain; the

wind about N.W. by N. all day; at times squally, rising to a force of

6 or 7 and sometimes dropping to a force of 2 or 3. The station at

Leigh excepted, all these places were to leeward of Shoeburyness. At

four other stations to leeward, varying in distance from 15.5 to 24.5

miles, nothing was heard, while at eleven stations to windward,

varying from 8 to 26 miles, the sounds were also inaudible. It was

found, indeed, that the sounds proceeding directly against the wind

did not penetrate much beyond 3 miles.

On the following day, viz. the 18th October, we proceeded to Dungeness

with the view of making a series of strict comparative experiments

with gun-cotton and cotton-powder. Rockets containing 8 oz, 4 oz, and

2 oz. of gun-cotton had been prepared at the Royal Arsenal; while

others, containing similar quantities of cotton-powder, had been

supplied by the Cotton-powder Company at Faversham. With these were

compared the ordinary 18-pounder gun, which happened to be mounted at

Dungeness, firing the usual charge of 3 lbs. of powder, and a syren.

From these experiments it appeared that the guncotton and

cotton-powder were practically equal as producers of sound.

The effectiveness of small charges was illustrated in a very striking

manner, only a single unit separating the numerical value of the 8-oz.

rocket from that of the 2-oz. rocket. The former was recorded as 6.9

and the latter as 5.9, the value of the 4-oz. rocket being

intermediate between them. These results were recorded by a number of

very practised observers on board the 'Galatea.' They were completely

borne out by the observations of the Coastguard, who marked the value

of the 8-oz rocket 6-1, and that of the 2-oz. rocket 5.2. The

18-pounder gun fell far behind all the rockets, a result, possibly, to

be in part ascribed to the imperfection of the powder. The

performance of the syren was, on the whole, less satisfactory than

that of the rocket. The instrument was worked, not by steam of 70

lbs. pressure, as at the South Foreland, but by compressed air,

beginning with 40 lbs. and ending with 30 lbs. pressure. The trumpet

was pointed to windward, and in the axis of the instrument the sound

was about as effective as that of the 8-oz. rocket. But in a

direction at right angles to the axis, and still more in the rear of

this direction, the syren fell very sensibly behind even the 2-oz.

rocket.

These are the principal comparative trials made between the gun-cotton

rocket and other fog-signals; but they are not the only ones. On the

2nd of August, 1877, for example, experiments were made at Lundy

Island with the following results. At 2 miles distant from the

firing-point, with land intervening, the 18-pounder, firing a 3-lb.

charge, was quite unheard. Both the 4-oz. rocket and the 8-oz.

rocket, however, reached an elevation which commanded the acoustic

shadow, and yielded loud reports. When both were in view the rockets

were still superior to the gun. On the 6th of August, at St. Ann's,

the 4-oz. and 8-oz. rockets proved superior to the syren. On the

Shambles Light-vessel, when a pressure of 13 lbs. was employed to

sound the syren, the rockets proved greatly superior to that

instrument. Proceeding along the sea margin at Flamboro' Head, Mr.

Edwards states that at a distance of 1.25 mile, with the 18-pounder

previously used as a fog-signal hidden behind the cliffs, its report

was quite unheard, while the 4-oz. rocket, rising to an elevation

which brought it clearly into view, yielded a powerful sound in the

face of an opposing wind.

On the evening of February 9th, 1877, a remarkable series of

experiments were made by Mr. Prentice at Stowmarket with the

gun-cotton rocket. From the report with which he has kindly furnished

me I extract the following particulars. The first column in the

annexed statement contains the name of the place of observation, the

second its distance from the firing-point, and the third the result

observed:

Stoke Hill, Ipswich 10 miles Rockets clearly seen and sounds

distinctly heard 53 seconds after the flash.

Melton 15 miles Signals distinctly heard. Thought at

first that sounds were reverberated

from the sea.

Framlingham 18 miles Signals very distinctly heard, both in

the open air and in a closed room.

Wind in favour of sound.

Stratford. 19 miles St. Andrews Reports loud; startled

pheasants in a cover close by.

Tuddenham. 10 miles St. Martin Reports very loud; rolled

away like thunder.

Christ Church Park. 11 miles Report arrived a little more than a

minute after flash.

Nettlestead Hall 6 miles Distinct in every part of observer's

house. Very loud in the open air.

Bildestone 6 miles Explosion very loud, wind against sound.

Nacton 14 miles Reports quite distinct--mistaken by

inhabitants for claps of thunder.

Aldboro' 25 miles Rockets seen through a very hazy

atmosphere; a rumbling detonation heard.

Capel Mills 11 miles Reports heard within and without the

observer's house. Wind opposed to sound.

Lawford 15.5 miles Reports distinct: attributed to

distant thunder.

In the great majority of these cases, the direction of the sound

enclosed a large angle with the direction of the wind. In some cases,

indeed, the two directions were at right angles to each other. It is

needless to dwell for a moment on the advantage of possessing a signal

commanding ranges such as these.

The explosion of substances in the air, after having been carried to a

considerable elevation by rockets, is a familiar performance. In

1873, moreover, the Board of Trade proposed a light-and-sound rocket

as a signal of distress, which proposal was subsequently realized, but

in a form too elaborate and expensive for practical use. The idea of

a gun-cotton rocket fit for signalling in fogs is, I believe, wholly

due to Sir Richard Collinson, the Deputy Master of the Trinity House.

Thanks to the skilful aid given by the authorities of Woolwich, by Mr.

Prentice, and Mr. Brock, that idea is now an accomplished fact; a

signal of great power, handiness, and economy, being thus placed at

the service of our mariners. Not only may the rocket be applied in

association with lighthouses and lightships, but in the Navy also it

may be turned to important account. Soon after the loss of the

'Vanguard' I ventured to urge upon an eminent naval officer the

desirability of having an organized code of fog-signals for the fleet.

He shook his head doubtingly, and referred to the difficulty of

finding room for signal guns. The gun-cotton rocket completely

surmounts this difficulty, It is manipulated with ease and rapidity,

while its discharges may be so grouped and combined as to give a most

important extension to the voice of the admiral in command. It is

needless to add that at any point upon our coasts, or upon any other

coast, where its establishment might be desirable, a fog-signal

station might be extemporised without difficulty.

*****

I have referred more than once to the train of echoes which

accompanied the explosion of gun-cotton in free air, speaking of them

as similar in all respects to those which were described for the first

time in my Report on Fog-signals, addressed to the Corporation of

Trinity House in 1874. [Footnote: See also 'Philosophical

Transactions' for 1874, p. 183.] To these echoes I attached a

fundamental significance. There was no visible reflecting surface

from which they could come. On some days, with hardly a cloud in the

air and hardly a ripple on the sea, they reached a magical intensity.

As far as the sense of hearing could judge, they came from the body of

the air in front of the great trumpet which produced them. The

trumpet blasts were five seconds in duration, but long before the

blast had ceased the echoes struck in, adding their strength to the

primitive note of the trumpet. After the blast had ended the echoes

continued, retreating further and further from the point of

observation, and finally dying away at great distances. The echoes

were perfectly continuous as long as the sea was clear of ships,

'tapering' by imperceptible gradations into absolute silence. But

when a ship happened to throw itself athwart the course of the sound,

the echo from the broadside of the vessel was returned as a shock

which rudely interrupted the continuity of the dying atmospheric

music.

These echoes have been ascribed to reflection from the crests of the

sea-waves. But this hypothesis is negatived by the fact, that the

echoes were produced in great intensity and duration when no waves

existed--when the sea, in fact, was of glassy smoothness. It has been

also shown that the direction of the echoes depended not on that of

waves, real or assumed, but on the direction of the axis of the

trumpet. Causing that axis to traverse an arc of 210°, and the

trumpet to sound at various points of the arc, the echoes were always,

at all events in calm weather, returned from that portion of the

atmosphere towards which the trumpet was directed. They could not,

under the circumstances, come from the glassy sea; while both their

variation of direction and their perfectly continuous fall into

silence, are irreconcilable with the notion that they came from fixed

objects on the land. They came from that portion of the atmosphere

into which the trumpet poured its maximum sound, and fell in intensity

as the direct sound penetrated to greater atmospheric distances.

The day on which our latest observations were made was particularly

fine. Before reaching Dungeness, the smoothness of the sea and the

serenity of the air caused me to test the echoing power of the

atmosphere. A single ship lay about half a mile distant between us

and the land. The result of the proposed experiment was clearly

foreseen. It was this. The rocket being sent up, it exploded at a

great height; the echoes retreated in their usual fashion, becoming

less and less intense as the distances of the invisible surfaces of

reflection from the observers increased. About five seconds after the

explosion, a single loud shock was sent back to us from the side of

the vessel lying between us and the land. Obliterated for a moment by

this more intense echo the aerial reverberation continued its retreat,

dying away into silence in two or three seconds afterwards. [Footnote:

The echoes of the gun fired on shore this day were very brief; those

of the 12-oz. gun-cotton rocket were 12" and those of the 8-oz.

cotton-powder rocket 11" in duration.]

I have referred to the firing of an 8-oz. rocket from the deck of the

'Galatea' on March 8, 1877, stating the duration of its echoes to be

seven seconds. Mr. Prentice, who was present at the time, assured me

that in his experiments similar echoes had been frequently heard of

more than twice this duration. The ranges of his sounds alone would

render this result in the highest degree probable.

To attempt to interpret an experiment which I have not had an

opportunity of repeating, is an operation of some risk; and it is not

without a consciousness of this that I refer here to a result

announced by Professor Joseph Henry, which he considers adverse to the

notion of aerial echoes. He took the trouble to point the trumpet of

a syren towards the zenith, and found that when the syren was sounded

no echo was returned. Now the reflecting surfaces which give rise to

these echoes are for the most part due to differences of temperature

between sea and air. If, through any cause, the air above be chilled,

we have descending streams--if the air below be warmed, we have

ascending streams as the initial cause of atmospheric flocculence. A

sound proceeding vertically does not cross the streams, nor impinge

upon the reflecting surfaces, as does a sound proceeding horizontally

across them. Aerial echoes, therefore, will not accompany the

vertical sound as they accompany the horizontal one. The experiment,

as I interpret it, is not opposed to the theory of these echoes which

I have ventured to enunciate. But, as I have indicated, not only to

see but to vary such an experiment is a necessary prelude to grasping

its full significance.

In a paper published in the 'Philosophical Transactions' for 1876,

Professor Osborne Reynolds refers to these echoes in the following

terms Without attempting to explain the reverberations and echoes

which have been observed, I will merely call attention to the fact

that in no case have I heard any attending the reports of the rockets,

[Footnote: These carried 12 oz. of gunpowder, which has been found by

Col. Fraser to require an iron case to produce an effective

explosion.] although they seem to have been invariable with the guns

and pistols. These facts suggest that the echoes are in some way

connected with the direction given to the sound. They are caused by

the voice, trumpets, and the syren, all of which give direction to the

sound; but I am not aware that they have ever been observed in the

case of a sound which has no direction of greatest intensity.' The

reference to the voice, and other references in his paper, cause me to

think that, in speaking of echoes, Professor Osborne Reynolds and

myself are dealing with different phenomena. Be that as it may, the

foregoing observations render it perfectly certain that the condition

as to direction here laid down is not necessary to the production of

the echoes.

There is not a feature connected with the aerial echoes which cannot

be brought out by experiments in the air of the laboratory. I have

recently made the following experiment: A rectangle, x Y (p. 331),

22 inches by 12, was crossed by twenty-three brass tubes (half the

number would suffice and only eleven are shown in the figure), each

having a slit along it from which gas can issue. In this way

twenty-three low flat flames were obtained. A sounding reed a fixed

in a short tube was placed at one end of the rectangle, and a

'sensitive flame,' [Footnote: Fully described in my 'Lectures on

Sound,' 3rd edition, p. 227.] f, at some distance beyond the other

end. When the reed sounded, the flame in front of it was violently

agitated, and roared boisterously. Turning on the gas, and lighting

it as it issued from the slits, the air above the flames became so

heterogeneous that the sensitive flame was instantly stilled, rising

from a height of 6 inches to a height of 18 inches. Here we had the

acoustic opacity of the air in front of the South Foreland strikingly

imitated. [Footnote: Lectures on Sound, 3rd ed, p. 268.] Turning off

the gas, and removing the sensitive flame to f, some distance behind

the reed, it burned there tranquilly, though the reed was sounding.

Again lighting the gas as it issued from the brass tubes, the sound

reflected from the heterogeneous air threw the sensitive flame into

violent agitation. Here we had imitated the aerial echoes heard when

standing behind the syren-trumpet at the South Foreland. The

experiment is extremely simple, and in the highest degree impressive.

Fig. 11.

*****

The explosive rapidity of dynamite marks it as a substance specially

suitable for the production of sound. At the suggestion of Professor

Dewar, Mr. McRoberts has carried out a series of experiments on

dynamite, with extremely promising results. Immediately after the

delivery of the foregoing lecture I was informed that Mr. Brock

proposed the employment of dynamite in the Collinson rocket.

********************

XI. ON THE STUDY OF PHYSICS.

[Footnote: From a lecture delivered in the Royal Institution of Great

Britain in the Spring of 1854.]

I HOLD in my hand an uncorrected proof of the syllabus of this course

of lectures, and the title of the present lecture A there stated to be

'On the Importance of the Study of Physics as a Means of Education.'

The corrected proof, however, contains the title: 'On the Importance

of the Study of Physics as a Branch of Education.' Small as this

editorial alteration may seem, the two words suggest two radically

distinct modes of viewing the subject before us. The term Education

is sometimes applied to a single faculty or organ, and if we know

wherein the education of a single faculty consists, this will help us

to clearer notions regarding the education of the sum of all the

faculties, or of the mind. When, for example, we speak of the

education of the voice, what do we mean? There are certain membranes

at the top of the windpipe which throw into vibration the air forced

between them from the lungs, thus producing musical sounds. These

membranes are, to some extent, under the control of the will, and it

is found that they can be so modified by exercise as to produce notes

of a clearer and more melodious character. This exercise we call the

education of the voice. We may choose for our exercise songs new or

old, festive or solemn; the education of the voice being the object

aimed at, the songs may be regarded as the means by which this

education is accomplished. I think this expresses the state of the

case more clearly than if we were to call the songs a branch of

education. Regarding also the education of the human mind as the

improvement and development of the mental faculties, I shall consider

the study of Physics as a means towards the attainment of this end.

From this point of view, I degrade Physics into an implement of

culture, and this is my deliberate design.

The term Physics, as made use of in the present Lecture, refers to

that portion of natural science which lies midway between astronomy

and chemistry. The former, indeed, is Physics applied to 'masses of

enormous weight,' while the latter is Physics applied to atoms and

molecules. The subjects of Physics proper are therefore those which

lie nearest to human perception: light and heat, colour, sound,

motion, the loadstone, electrical attractions and repulsions, thunder

and lightning, rain, snow, dew, and so forth. Our senses stand

between these phenomena and the reasoning mind. We observe the fact,

but are not satisfied with the mere act of observation: the fact must

be accounted for--fitted into its position in the line of cause and

effect. Taking our facts from Nature we transfer them to the domain

of thought: look at them, compare them, observe their mutual relations

and connexions, and bringing them ever clearer before the mental eye,

finally alight upon the cause which unites them. This is the last act

of the mind, in this centripetal direction--in its progress from the

multiplicity of facts to the central cause on which they depend. But,

having guessed the cause, we are not yet contented. We set out from

the centre and travel in the other direction. If the guess be true,

certain consequences must follow from it, and we appeal to the law and

testimony of experiment whether the thing is so. Thus is the circuit

of thought completed,--from without inward, from multiplicity to

unity, and from within outward, from unity to multiplicity. In thus

traversing both ways the line between cause and effect, all our

reasoning powers are called into play. The mental effort involved in

these processes may be compared to those exercises of the body which

invoke the co-operation of every muscle, and thus confer upon the

whole frame the benefits of healthy action.

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