The reason why we so seldom see the bottom of the sea, or of a pure

lake, where the depth is not beyond the powers of natural vision, is

not that the rays of light reflected from the objects at the bottom

are so feeble as to be imperceptible to our sense, from their passage

through the denser medium of the water, but from the irregular

refractions given to the rays in passing out of the water into the

air, caused by the constant ripple or motion of the surface of the

water, where that refraction takes place. Reflections of light from

the surface also add to the difficulty; and before we can with any

just hope expect to see the objects distinctly at the bottom, these

obstructions must be removed.

This is done to a very great extent by the use of the instrument which

forms the subject of this notice; the tube serves to screen the eyes

from reflections, and the water being in contact with the glass plate,

all ripple is got rid of, so that the spectator, looking down the

tube, sees all objects at the bottom, whose reflective powers are able

to send off rays of sufficient intensity to be impressed on the

retina, after suffering the loss of light caused by the absorbing

power of the water, which obeys certain fixed laws, proportionate to

the depth of water passed through; for as light passing through pure

sea-water loses half its intensity for each 15 feet through which it

passes,[49] we must, from this cause alone, at a certain depth lose

sight of objects of the brightest lustre. The perfect purity of the

water, and its freedom from all muddy particles floating in it, form

an important element in the effective use of the water-telescope; for

example, in the Frith of Forth, and similar estuaries, where the

influx and reflux of the tide keep particles of mud in constant

motion, the instrument is of little or no use; for these act in

exactly the same way in limiting our vision through water, as a fog

does through the air: it is therefore only in the pure waters of our

northern and western shores that this contrivance is applied with any

advantage; and in such situations we can speak of its powers with

confidence. In a trial made with the instrument last autumn on the

west coast of Scotland, the bottom was distinctly seen (a white

bottom) at a depth of 12 fathoms; and on a black, rocky bottom, at 5

fathoms under water, objects were so distinctly seen that the parts of

a wreck were taken up--the exact place of which was not known previous

to its use. In these experiments a lenticular form of glass was made

use of at the bottom of the tube, having a plane surface to the water,

but no great or marked advantage was observable from this

construction. With respect to the history of this contrivance for

viewing the bottom of the sea, we are unable to assign any particular

date: so far as our information goes, it has been in use from a very

remote period. We are informed that it is in general use in

seal-shooting along our northern and western islands, where, sometimes

in the form of an ordinary washing-tub, with a piece of glass fixed in

its bottom, the shot-seal was looked for, and the grappling-hook let

down to bring him to the surface. It may not be generally known, that

in seal-shooting, the shot or wounded seal always seeks the bottom,

from which he never rises after death, till washed ashore by the

action of the sea: it is only when the fatal ball deprives him of the

power of diving that he is ever found at the surface. In such

employments, therefore, the use of this instrument, however modified,

must form an important auxiliary to the best rifle. Throwing oil over

the surface of the water is used in the same pursuits; but this only

so far stills the ripple, leaving the reflections. Our eminent

engineer, Mr Robert Stevenson, made use of the water-telescope more

than 30 years ago, in works connected with harbour improvement in the

north of Scotland; it has also been used to examine the sand-banks,

&c., at the bottom of the River Tay, but in this case the mud

prevented its use in any considerable depth of water. To obviate this

difficulty, the construction was modified thus: by making the tube of

considerable length, and placing the glass at the lower end, this tube

was thrust through the water till within a few feet of the bottom,

acting as a cofferdam to set aside the dirty water, and enable the

bottom to be seen; but in this method of application it was found very

difficult to hold the tube down in the water from its buoyant power,

and we are informed by Mr Thomas Stevenson, C. E., that, he understood

from this cause its use had been discontinued. He suggested a simple

remedy; viz., to fill up the empty tube with pure water. We are

indebted to Mr Mitchell, the gentleman already mentioned, for having

brought this instrument into notice in the public prints, under the

name of Norwegian water-telescope, on the shores of which country it

is stated to be much used in fishing--in particular, that of the

herring; but the herring-fishers on the east coast of Scotland inform

us, that they require no such auxiliary, as, from the surrounding

elevated grounds, they can tell the position of the shoal, and, from

their motions seen from such situations, they know where they are to

be found when they go out a-fishing.[50]

Footnote 49: Leslie's Elements of Nat. Phil., p. 19.

Footnote 50: _Norwegian Water-Telescope._

The water-telescope is thus noticed in a very promising

periodical, the American Annual of Scientific Discovery, just

published, of which a copy reached us a few days ago.--ED. _Phil.

Journal_.

The water-telescope is an instrument which the people of Norway

have found of so great utility, that there is scarcely a single

fishing-boat without one of three or four feet in length, which

they carry in their boats with them when they go a-fishing. When

they reach the fishing-grounds, they immerse one end of this

telescope in the water, and look through the glass, which shews

objects some ten or fifteen fathoms deep as distinctly as if they

were within a foot of the surface. When a shoal of fish comes

into their bays, the Norwegians instantly prepare their nets, man

their boats, and go out in pursuit. The first process is minutely

to survey the ground with their glasses, and where they find the

fish swarming about in great numbers, they give the signal, and

surround the fish with their large draught-nets, and often catch

them in hundreds at a time. Without these telescopes their

business would often prove precarious and unprofitable; as the

fish, by these glasses, are as distinctly seen in the deep, clear

sea of Norway, as gold-fish in a crystal jar. This instrument is

not only used by the fishermen, but is also found aboard the navy

and coasting-vessels of Norway. When their anchors get into foul

ground, or their cables warped on a roadstead, they immediately

apply the glass, and, guided by it, take steps to put all to

rights, which they could not do so well without the aid of the

rude and simple instrument, which the meanest fisherman can make

up with his own hands, without the aid of a craftsman. This

instrument has been lately adopted by the Scotch fishermen on the

Tay, and, by its assistance, they have been enabled to discover

stones, holes, and uneven ground, over which their nets travel,

and have found the telescope answer to admiration, the minutest

object in twelve feet of water being as clearly seen as on the

surface. We see no reason why it could not be used with advantage

in the rivers and bays of the United States.

_Experimental Investigations to Discover the Cause of the Change

which takes place in the Standard Points of Thermometers._

By JOHN ADIE, F.R.S.E., F.R.S.S.A.

Communicated by the Author.

It has long been known to experimentalists that, in thermometers

constructed with the greatest care, a change takes place after a lapse

of time in the standard points, as given by the melting of ice and

boiling of water under a fixed pressure; on this account it has been

recommended by most writers, where the employment of thermometers is

treated of, that they should from time to time be compared one with

another, and also at the freezing point. This change is a rising of

the mercury in the tube, so that, after a length of time, the mercury

will not sink to the point laid off in the construction of the

instrument. To investigate to what cause this change was due, formed

the object of my experiments: Was it a change in the glass of which

the bulbs are formed, or in the mercury with which they are filled? I

was aware that thermometers filled with alcohol were not subject to

this change, which would lead to the inference, that the change was in

the mercury and not the glass; but then, in the spirit-thermometer,

air is left above the column of spirit, whereas, in those constructed

with mercury, the air is expelled, and there is a vacuum above the

column; consequently, the bulb is pressed together with the force of

an atmosphere on all sides; might not this force, acting for a length

of time, cause some small alteration in the arrangement of the

particles forming the glass of the bulb?

This is the explanation accepted by most of the Italian and French

writers on this subject. Some suppose that the mercury may contain air

and moisture within its particles; but such a hypothesis I think

inadmissible, as in the case of a vacuum over the mercury, these

particles would seek the void, and cause rather a depression than a

rising of the freezing point. Mr Daniell, in his Essay on Climate,

adopts the same view; and Sir John Herschel, in his article "Heat," in

the Encyclopædia Metropolitana, says: "The freezing point upon the

mercurial thermometer has been supposed to undergo some slight

variation, so as to appear too low upon the scales of those

instruments which have been long made; and it is said that, in such

cases, the just indication was again recovered by breaking off the end

of the stem, so as to admit atmospheric air." But, as I had observed

that the change went on for a time only, after which it ceased, and

that it affected thermometers sealed with air over the mercury, as

well as those with a vacuum, I undertook the following experiments:--

In September 1848 I made four thermometers having long degrees,--such

that 1/10° might be easily noted, constructed of the same draft of

glass tube; two of these I placed in boiling water, and kept them at

that temperature for a week: my object in this was to learn if any

change in the form of the bulb would take place from this slow process

of annealing, as glass is known to undergo some change from such

exposure.

The four thermometers were now filled with pure mercury: two of these

were sealed with a vacuum over the mercury; one tube that had been

boiled, and the other not: the other two tubes were sealed with air

over their columns, and the freezing points of all were marked on the

tubes; after which they were placed in a window freely exposed to

light, where they were left till January 1849--a space of four

months--when they were again placed in melting ice, and the freezing

points marked; they had risen ·24°, ·24°, ·20°, ·06° parts of a

degree. The whole four thermometers were now placed in boiling water,

and kept there for a week, when the freezing points were again

observed to have risen respectively ·48°, ·41°, ·50°, ·45°.

The instruments were now left exposed to light as at first; and, in

January 1850, the freezing points were again observed, when they were

found to have farther risen ·12°, ·18°, ·20°, ·13°; and, lastly, they

were observed in May 1850, when no change from last observation was

notable.

The whole amount of rising of the freezing point in these four

thermometers, after a lapse of eighteen months, is respectively ·84°,

·83°, ·90°, ·65°; and these changes may be the full amount that would

take place were the instruments observed after a greater lapse of

time. From my experience, I know that there is a period after which no

change takes place; but, from the method in which these experiments

have been conducted, I am not at present in a condition to assign a

time; moreover, it is evident that this period will be much modified

by circumstances. The results above stated form the following Table:--

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

| No.| Description | Value of | Observed | Rise after | | |

| | of |one Degree|rise, Jan. | having | Rise at | Total |

| |Thermometer. | of Fahr. | 1849. |been boiled |Jan. 1850.| rise. |

| | | | |for a week. | | |

|----+-------------+----------+-----------+------------+----------+-------|

| { | Sealed in | } | | | | |

|1.{ | vacuum, | } 0·166 | 0·24 | 0·48 | 0·12 | 0·84 |

| { | not boiled. | } | | | | |

|----+-------------+----------+-----------+------------+----------+-------|

| { | Sealed in | } | | | | |

|2.{ | vacuum and | } 0·168 | 0·24 | 0·41 | 0·18 | 0·83 |

| { | boiled. | } | | | | |

|----+-------------+----------+-----------+------------+----------+-------|

| { | Sealed with | } | | | | |

|3.{ | air, not | } 0·199 | 0·20 | 0·50 | 0·20 | 0·90 |

| { | boiled. | } | | | | |

|----+-------------+----------+-----------+------------+----------+-------|

| { |Sealed with | } | | | | |

|4.{ |air, boiled. | } 0·154 | 0·06 | 0·45 | 0·13 | 0·65 |

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

From inspection of the Table, no very remarkable difference is

observable in the rising of these four instruments. No. 4 appears to

have risen less during the first period, but goes along with the

others afterwards. The effect of exposure to the temperature of

boiling water shews that, under high temperature, the change goes on

much faster than at the ordinary temperature of the air; from the

Table it will be observed, that about twice the amount of change was

caused by the boiling of the thermometers for a week, than had taken

place between the first and second observations, a period of four

months.

It does not appear that the boiling of the thermometer tubes for eight

days, previous to their being filled with mercury, had produced any

change on the form of the bulbs; we should at least infer this from

the change in their freezing points keeping pace so nearly with those

which had not been boiled.

I now come to the concluding experiment with these instruments, and,

it appears to me most interesting and anomalous. The four tubes being

placed in pounded ice, the columns stood at the points indicated in

the last column of the Table; in this situation the tops of the tubes

were broken off, so as to admit the free pressure of the air, and

instantly the thermometers fell, in the order of their numbers, ·54,

·43, ·40, ·35 of a degree, now indicating on their scales +·30, +·40,

+·50, +·35. The remarkable features shewn by this experiment are;

first, that the two thermometers sealed with vacuum, and the two

having air over their columns, should have risen nearly equally, when

two had their bulbs pressed with the whole force of an atmosphere,

while the other two had no pressure externally, farther than that

caused from changes in the pressure of the atmosphere. Next, that on

being opened, those with air over them should have started down nearly

as much as those with a vacuum; and on all these appears a permanent

change from three to five-tenths of a degree. I confess that I am very

much at a loss to account for these singular changes; atmospheric

pressure on the bulbs would account for the change in those sealed

with a vacuum; for we can easily suppose that a permanent form had

been taken from long exposure to that pressure by the glass forming

the bulbs: besides this permanent form, there appears to have been a

spring inwards, which instantly sprung out on removal of the pressure

by the admission of air over the mercury; but the same reasoning will

not apply to the thermometers having air over the mercury; and before

I attempt to make any suggestions as to the cause of these changes, I

propose to institute the following experiments. Having had three

thermometers blown and filled with mercury, I shall make one with a

perfect vacuum over the mercury, the next with air over it, and the

third with air condensed over it; and, noting the changes that may go

on in these, I hope to be able to assign a cause or causes for the

change. It is argued by some continental writers on this subject that

the reason why we do not perceive any change in the freezing point in

spirit-thermometers is from the great expansion of spirit above

mercury, volume for volume, thereby requiring a much smaller mass of

fluid to give the same length of a degree: this I propose to test by

making a thermometer with the same size of tube and bulb as those to

be experimented on with mercury. In mentioning these experiments to

Professor Forbes, he kindly put me in possession of some

spirit-thermometers, one of these, made in 1837, having a very large

bulb--this, with three others, shewed no change in the places of their

freezing points.

_Observations on the Discovery, by_ Professor LEPSIUS, _of Sculptured

Marks on Rocks in the Nile Valley in Nubia; indicating that,

within the historical period, the river had flowed at a higher

level than has been known in Modern Times_.

By LEONARD HORNER, Esq., F.R.S.S. L. & E., F.G.S., &c.

Communicated by the Author. With a Plate.

The recent archaeological researches of Professor Lepsius in Egypt,

and the Valley of the Nile, in Nubia, have given a deserved celebrity

and authority to his name, among all who take an interest in the early

history of that remarkable portion of the Old World. While examining

the ruins of a fortress, and of two temples of high antiquity at

Semne, in Nubia, he discovered marks cut in the solid rocks, and in

the foundation-stones of the fortress, indicating that, at a very

remote period in the annals of the country, the Nile must have flowed

at a level considerably above the highest point which it has ever

reached during the greatest inundations in modern times. This

remarkable fact would possess much geological interest with respect to

any great river, but it does so especially in the case of the Nile.

Its annual inundations, and the uniformity in the periods of its rise

and fall, have been recorded with considerable accuracy for many

centuries; the solid matter held in suspension in its waters, slowly

deposited on the land overflowed, has been productive of changes in

the configuration of the country, not only in times long antecedent to

history, but throughout all history, down to the present day. Of no

other river on the earth's surface do we possess such or similar

records; and moreover, the Nile, and the changes it has produced on

the physical character of Egypt, are intimately associated with the

earliest records and traditions of the human race. Everything,

therefore, relating to the physical history of the Nile Valley must

always be an object of interest; but the discovery of Professor

Lepsius is one peculiarly deserving the attention of the geologist;

for he does not merely record the facts of the markings of the former

high level of the river, but he infers from these marks, that since

the reign of Moeris, about 2200 years before our era, the entire bed

of the Nile, in Lower Nubia, must have been excavated to a depth of

about 27 feet; and he further speculates as to the process by which he

believes the excavation to have been effected.

It will be convenient, before entering upon the observations I have to

offer upon the cause assigned by Professor Lepsius for the former

higher levels of the Nile indicated by these marks, that I should give

the description of the discovery itself, by translating Dr Lepsius's

own account of it, in letters which he addressed to his friends,

Professors Ehrenberg and Böckh of Berlin, from the island of Philæ, in

September 1844.[51]

Footnote 51: Bericht über die zur Bekantmachung geeigneten

Verhandlungen der Königl. Preuss. Akademie der Wissenshaften zu

Berlin. Aus dem Jahre 1844.

"You may probably remember, when travelling to Dongola on the

Lybian side of the Nile, and in passing through the district of

Batn el hagér, that one of the most considerable of the cataracts

of the country occurs near Semne, a very old fortress, with a

handsome temple, built of sandstone, in a good state of

preservation; the track of the caravan passing close to it, partly

over the 4000-year-old artificial road. The track on the eastern

bank of the river is higher up, being carried through the hills;

and you must turn off from it at this point in order to see the

cataract. This Nile-pass, the narrowest with which I am

acquainted, according to the measurement of Hr. Erbkam, is 380

metres (1247 English feet) broad;[52] and both in itself, and on

account of the monuments existing there, is one of the most

interesting localities in the country, and we passed twelve days

in its examination.

Footnote 52: The breadth of the river itself. See Letter to Hr.

Böckh, p. 27.

"The river is here confined between steep rocky cliffs on both

sides, whose summits are occupied by two fortresses of the most

ancient and most massive construction, distinguishable at once

from the numerous other forts, which, in the time of the Nubian

power in this land of cliffs, were erected on most of the larger

islands, and on the hills commanding the river. The cataract (or

rapid) derives its name of Semne from that of the higher of the

two fortresses on the western bank; that on the opposite bank, as

well as a poor village lying somewhat south of it, is called

Kumme. In both fortresses the highest and best position is

occupied by a temple, built of huge blocks of sandstone, of two

kinds, which must have been brought from a great distance through

the rapids; for, southward, no sandstone is found nearer than

Gebel Abir, in the neighbourhood of Amara and the island of Sai

(between 80 and 90 English miles), and northward, there is none

nearer than the great division of the district at Wadi Haifa (30

miles distant.)

"Both temples were built in the time of Tutmosis III., a king of

the 18th dynasty, about 1600 years before Christ; but the

fortresses in which they stand are of a more ancient date. The

foundations of these are granite blocks of Cyclopian dimensions,

resting on the rock, and scarcely inferior to the rock itself in

durability. They were erected by the first conqueror of the

country, King Sesuatesen III., of the 12th dynasty, in order to

command the river, so easily done in so narrow a gorge. The

immediate successor of this king was Amenemha III., the Moeris of

the Greeks: he who accomplished the gigantic work of forming the

artificial lake of Moeris, in the Fayoum, and from whose time--the

most flourishing of the whole of the old Egyptian kingdom--the

risings of the Nile in successive years, doubtless by means of

regular markings, as indeed Diodorus tells, remained so well

known, that, according to Herodotus, they were recorded in

distinct numbers from the time of Moeris. It appears that this

provident king, occupied with great schemes for the welfare of his

country, considered it of great importance that the rising of the

Nile on the most southern border of his kingdom should be

observed, and the results forthwith communicated widely in other

parts of the land, to prepare the people for the inundations. The

gorge at Semne offered greater advantages for this object than any

other point; because the river was there securely confined by

precipitous rocky cliffs on each side. With the same view he had

doubtless caused Nilometers to be fixed at Assuan and other

suitable places; for without a comparison with these, the

observations at Semne could be of little use.

The Edinburgh New Philosophical Journal, Vol. XLIX April-October 1850 · 第 12 / 20 段