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shown fail to recognize the bird at all. They speak also of another flightless bird by the name of Mehunui. This bird, one old and very intelligent Moriori informed me, was the same as the Maoris called Kakapo. Mr. Alexander Shand, an old resident in the Chatham Islands, and the sole European living versed in Moriori customs and traditions, and capable of speaking their language with fluency, also confirmed this information, and told me that the Kakapo (according to the Morioris) was very abundant in the islands prior to 1836. He himself in the early days had seen their burrows often. I had observed, while collecting, several Psittacine bones, and on learning this fact I felt sure that those I had picked up and packed away must belong to Stringops. On my arrival here, however, I find so far that there are no Kakapo bones in the collection, the Psittacine bones being the head and beaks of Nestor notabilis, the Kea. I have as yet had time to do no more than run through the collection I have brought back; but there appear to be in it several large Ralline tibiæ of species unknown to me. I am looking forward to another opportunity of thoroughly exploring these interesting islands with more time at my disposal than I could afford on this occasion. HENRY O. FORBES.

Canterbury Museum, February 23.

Pigments of Lepidoptera.

A LETTER of mine on the subject of butterfly pigments was published so recently in NATURE (December 31, 1891, p. 197) that I hesitate to ask for further space at the present time. But the appearance of Mr. Perry Coste's articles, together with the tone of some remarks made by him at the close of the last article, lead me to venture upon a few words, partly in criticism of a theory he advances, and partly (though this is less important) in claim of priority, since Mr. Coste does not do me the honour to refer to my work on the subject.

The chief generalization which Mr. Coste bases upon his experiments is that which he terms the "reversion effect," that is to say, the production of yellows from reds by the action of acids, and the restoration of the former by neutralization and other means. The theory that he advances to explain these phenomena-namely, that the red body acts as a base, and forms with acids salts which are yellow-is quite untenable. As I have shown (Proceedings of the Chemical Society, June 1889; vide NATURE, vol. xl. p. 335), the soluble yellows are themselves acid bodies of quite definite composition. Indeed, as far back as 1871, Prof. Meldola called attention to the fact that the pigment of G. rhamni was soluble in water, and showed that its aqueous solution had an acid reaction. Mr. Coste has worked with D. eucharis; if he will dissolve the red pigment from the border of the hind wing of this insect in pure water, he will find that a yellow solution is the result, but that, if the solution be evaporated to dryness, the solid residue of pigment is red once more; showing that there is either the question of hydration to consider, or a weak combination of the yellow acid body with a base, which is dissociated in aqueous solution. At any rate, I have obtained from this red pigment of eucharis a silver compound which contains a percentage of metal exactly equal to that from the pigment of G. rhamni.

In 1889 I was able to predict possible constitutional formulæ for the acid yellow pigments, and am happy to say that recent careful combustions of their silver salts to a large extent confirm my original ideas. My results will be shortly published in

extenso.

Mr. Perry Coste's experiments are very useful as forming a method of classifying these lepidopterous pigments; but, if he will forgive me for saying so, they are of far too empirical a nature for any considerations as to the constitution of the bodies to be based upon them. As one who has for many years past spent a large portion of his time and no inconsiderable portion of his substance in obtaining a sufficiency of these pigments for analysis and investigation, Mr. Coste will forgive me if I do not respond to his invitation to leave him to continue his researches alone." It is hardly well for one investigator to say "hands off" to another, and I shall not imitate Mr. Coste in this matter; but will only express a hope that in his future work he will not confine himself to the immersion of the wings of his insects in strong and destructive reagents.

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I have lately been working at the genesis of these pigments in the pupæ, and might say something with regard to the nature of

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THE new edition of Prof. Everett's "C.G.S. System of Units" contains, at the very beginning, two misleading statements, based seemingly on a misapprehension of facts. In so valuable a work, such errors are to be deplored.

Pp. xiii. and xiv. give an account of weighings made at the International Bureau of Weights and Measures between certain "standard pounds" and the international standard of mass. From the statement as given, it would be inferred that there is room for doubt as to the relation between the British standard of mass and the international kilogramme.

The real facts are, that the standard pounds were only nominally "pounds"; they were standards with known corrections, which, however, have not been applied to the equivalents given on p. xiv.

The true relation of the Imperial pound to the international kilogramme is given in the Board of Trade Report of Proceedings under the Weights and Measures Act, 1884 (p. 4), according to which the Imperial pound = 453'5924277 grammes.

On p. 34 of "C.G. S. System of Units," Mr. Chaney's results of the weight of a cubic inch of water are discussed, and the conclusion is reached that Mr. Chaney's result differs by o'00125 from the theoretical relation between volume and mass of water in the metric system.

This result is obtained by comparing Mr. Chaney's results, without reduction to vacuo, with the mass of a cubic centimetre of water.

Mr. Chaney states that the standard air to which his result is reduced weighs 0'3077 grains per cubic inch. Therefore his result reduced to vacuo is: one cubic inch of water at 62° F. weighs 252 286 +0.308 = 252.594 grains.

If we take the value for the thermal expansion of water, in terms of the hydrogen thermometer scale, as determined at the International Bureau, we find the density of water at 16° 667 C., = 62° F., referred to its maximum density o'998861.

=

=

Using the equivalents I metre = 39'3700 inches, and I gramme = 15 43235639 grains, we obtain: one cubic inch of water at 62° F. weighs in vacuo 252 6045 grains; while Mr. Chaney found 252.594 as above given, a discrepancy of one part in 25,000 only, as compared with one part in 800, given by Prof. Everett. It is not clear from Mr. Chaney's statement whether his weight in air is against brass or other weights; therefore the vacuum reduction above applied is uncertain by a small amount. O. H. TITTMANN.

Washington, D.C., March 10.

MR. TITTMANN thinks the true relation is, without doubt1 pound = 453'5924277 grammes.

Prof. W. H. Miller determined it to be

I pound = 453'59265 grammes, which is the value given on the Card of Equivalents published by the Board of Trade. If the determination quoted by Mr. Tittmann from a Board of Trade Report of 1884 was made under such conditions as to render it authoritative, it is a pity it has been allowed to remain for eight years buried in a Bluebook. One would have expected some intimation of it to be given to scientific men through the Royal Society or in the pages

of NATURE.

As regards the three "standard pounds" which were compared with standards at the Bureau International in 1883, Mr. Tittmann says they had known corrections. This is not stated in the Travaux et Mémoires, where the account of the comparison is given. There is, however, in the case of the two which are of gilded bronze, a reference to a description of them by Prof. Miller in his paper on the standard pound (Phil. Trans. 1856), and, on turning to it, I find that their errors, as stated by him, do not agree even approximately with the determinations made at the Bureau. They differ even in the first significant figure of the error, which is the sixth figure of the entire value; so that, as far as this evidence goes, the five figures 45359 are all that are certain.

As regards the other matter referred to, Mr. Tittmann does not mention the publication in which "Mr. Chaney states that the standard air to which his result is reduced weighs 0*3077 grains per cubic inch." The only publication known to me is Mr. Chaney's paper in the Proceedings of the Royal Society, and it does not contain any such statement.

I have always been taught to regard a standard weight as a standard of mass, and therefore independent of such conditions as temperature, pressure, and the material in the other scale pan; whereas, it appears that Mr. Chaney, by direction of the Board of Trade, has made a determination which is only true for a particular density of the surrounding air, and a particular density of the weights in the other pan.

For scientific purposes a standard of reference should be free from variable elements, and should be of the utmost attainable simplicity. For commercial purposes determinations to six figures are frivolous.

Mr. Tittmann's reductions appear to contain two errors. Instead of adding the weight of a cubic inch of air, he ought to have added the difference between this and the weight of the air displaced by the weights in the opposite pan. Again, he takes the metre as 39 3700 inches, whereas Clarke's value is 39'370432, and Kater's 39'37079.

I have had some correspondence with Mr. Chaney since the publication of my new edition, and have had an erratum slip printed, which I trust you will allow me to subjoin, as it may be useful to several of your readers J. D. EVERETT.

5 Princess Gardens, Belfast, March 28.

Addenda and Corrigenda.

Page 63. In reducing Cailletet's experiments, '0000026 should have been added instead of 000 0039.

Page 77. Add-Violle's determination of velocity of sound is 331 100'I. Ann. de Chim. XIX. March, 1890.

Page 176, line 10. For Wuilleumeier, 1890, read Wuilleumier, 1890, Lippmann method.

At end of page 164, add-Expressing C in amperes, Rin ohms, and 7 in seconds, the heating effect in gramme-degrees is CRT 4'2 = 24C RT.

Page 35. Mr. Chaney's determination here quoted was not intended as a determination of the density of water, but of the apparent weight of water when weighed in air of density 001 216 84 against brass weights of density 8'143. The correcting factor for deducing the weight in vacuo or true density is 1001 0687, which will change the value 998 752 obtained in the text into 999 82, to compare with Tralles' '999 88.

Mr. Chaney's result is for distilled water deprived of air, and Tralles' appears to be for ordinary distilled water. According to results recently obtained by the Vienna Standards Commission (Wied. Ann., 1891, Part 9, p. 171), water deprived of air has the greater density, the difference being 000 0032 at o° C., and 000 0017 at 62° F. These differences are too small to affect the above comparison.

Influenza in America.

In my copy of "Johnson's Dictionary of the English Language in Miniature, to which are added an alphabetical account of the heathen deities and a copious chronological table of remarkable events, discoveries, and inventions, by the Rev. Joseph Hamilton, M. A., second American edition, Boston, 1806" (12mo, pp. 276), I find on p. 275, "Influenza in North America, 1647, 1655, 1697 98, 1732, 1737, 1747, 1756-57, 1761, 1772, 1781, 1789-90, 1802." It is quite possible that these dates are well known, but they are new to me, and may be of interest in connection with the recent epidemic. EDWARD S. HOLDEN.

Mount Hamilton, March 29.

DUST COUNTING ON BEN NEVIS.

meteorological problems which deal with clouds and precipitation, solar and terrestrial radiation, and in a general way with the diurnal and annual variations in the temperature and pressure of the atmosphere. Mr. Aitken's work in originating this branch of science, and in making and discussing numerous observations of the number of dust particles in the air of various places in this country, as well as on the Continent, at various altitudes, is pretty well known already (see NATURE, vol. xli. p. 394). Mr. Aitken's results and conclusions were looked upon as being of such importance as to warrant some of our leading meteorologists to apply to the Research Fund of the Royal Society for a grant to enable them to equip the Ben Nevis Observatory with Aitken's dust-counting apparatus. The application was successful, and instru ments were at once ordered, and in due time erected a the Observatory.

The

The apparatus consists of two dust counters, one a portable form for use in the open air, and the other a laboratory form for use inside the Observatory. latter is fixed in the middle room of the tower, and has pipes leading out to the free air, so that it is possible to observe with it in almost all sorts of weather and at any hour day or night. The principle on which these instruments are constructed, so as to make the tiny invisible particles of dust visible and easily countable, is pretty well known already. Briefly it is this. To make the particles visible, the air containing them is saturated with water vapour, and by a stroke of an air-pump it is thereafter cooled so much as to cause a condensation of the vapour on the particles, whereby these are thus made visible. Ordinary air is so dusty that if the receiver were full of such air it would be impossible to count the particles, and to make them easily countable the following process is resorted to. First, the chamber or receiver, whose capacity is accurately known, is filled with pure dustless air by means of an air-pump and filter. Then a fifth, a tenth, or any other fractional part of the amount of pure air inside is taken out, and the same amount of dusty air allowed in. In this way the density of the shower caused by condensation is completely under the observer's control. A small graduated stage is placed one centimetre from the top of the receiver, so that all the dust above this falls on to it, and by means of a magnifying glass all the particles on one or more of the small squares of the stage are easily counted. Then, by multiplying by the reciprocals of the various fractions used we arrive at the number of dust particles in a unit of the free dusty air. In making an observation, the mean of ten such tests is taken as the number of particles present for that time.

with the portable instrument in February 1890, and with Observations were begun at the Ben Nevis Observatory the other instrument in the following summer. During the whole of that year the work done was mainly preliminary, as great difficulty was experienced in getting the dust work to fit into the general routine of Observatory work. The dust inquiry is not like some other special inquiries, that can be prosecuted for a certain time, and then discontinued after definite positive or negative conclusions thereanent have been arrived at, but must, on the other hand, be carried on side by side with the other observations of meteorological phenomena, as pressure, temperature, humidity, &c., with any of which it is of equal importance, and having once been admitted into the general routine of meteorological observations it

WITHIN the last few years quite a new factor has must be kept on. This fact was soon seen on Ben Nevis

been introduced into the study of meteorologynamely, that which treats of the dust particles in the atmosphere, of the number of dust particles present in the air at any time, and the effect of dust in the air on climate and weather changes. It is now beginning to be recognized that the study of dust and its behaviour in the air forms the stepping-stone to the study of almost all

from the extraordinary variations that were observed in the dustiness of the air with changes of weather; and it was attempted to make continuous hourly observations of the dust as of the other elements. It was found, however, that this could not be done without crippling the general routine, this being as much as the two observers at the Observatory could well cope with. In February 1891

a system of three-hourly observations of the dust particles was started, and this has been kept up with but few nterruptions since. The dust observation is made immediately after the usual hourly set is completed, and it can thus be studied along with all the other hourly records in their relation to the prevailing weather.

A great many observations have in this way been accumulated during the past two years, but we have not had time for studying them in detail yet. A mere inspection, however, brings out some interesting points. One of these is the enormous variation that is observed in the number of dust particles, not only in the course of the year, but often in the course of a few hours. At sea-level the number of dust particles in the air at any time depends very much on the locality and on the wind, whether blowing from a polluted district or not. The mean of a number of observations made by Mr. Aitken at Kingairloch, in the west of Scotland, is 1600 particles per cubic centimetre. In London, on the other hand, he found 100,000 per cubic centimetre, and in Paris rather more. On Ben Nevis the mean is 696 per cubic centimetre, the maximum being 14,400 per cubic centimetre, and on several occasions the minimum fell to o. A general mean does not convey a fair idea of the dustiness of the air at the mountain-top, although it may do so for places at sea-level, because there is at the former place a great daily range in the number of dust particles, depending on the rise and fall of the air past the place of observation. If there is any marked variation at sea-level it is entirely of a different character. Below are the means, as well as the maxima and mimima, of all the months that have a fairly representative number of observations.

Number of Dust Particles per cubic centimetre on Ben Nevis.

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The above table shows that the Ben Nevis air contains most dust in spring, and it is probable that sea-level air is in this respect similar; the cause of this greater amount of dust in spring than at any other time of the year being the great annual westward motion of the whole atmosphere, or at least of a considerable depth of it, at that time of the year. In a recent paper on "The Winds of Ben Nevis" (Trans. R.S.E., vol. xxxvi. p. 537), it has been shown that this is one of the very few points in which the high- and low-level winds agree, viz. in the excess of easterly winds in spring. The above means for summer are probably too low, as that summer was exceptionally cold, and the general circulation was very abnormal, and that in the direction which would tend to give low dust values. The maximum, 14,400, was observed at I p.m. on April 11, 1891; and, as an instance of how very much the values change in a short time, at 8 a.m. that morning the number was only 350 per cubic centimetre, and by midnight it had again fallen to 600 per cubic centimetre. The daily variation is fairly well indicated from the three-hourly observations. For the months of March, April, and May, 1891, the following are the means for the eight hours of observation :

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Here there is a minimum indicated (526) at 4 a.m., and a maximum (1438) at 4 p.m. All the forenoon values are below the mean, and the evening values above it. It would appear that during the forenoon the summit of Ben Nevis is above the first or lowest cloud or dust stratum. About noon this stratum rises to the level of the summit, and during the afternoon hovers above it, and falls again late at night. From this it might be inferred that the summit is oftener clear of cloud in the early morning, and oftener enveloped in the afternoon. A table showing the number of times the top was clear during the last seven years shows that only about 30 per cent. is clear weather in which the summit is free from fog; but it does not show a daily variation as indicated by the dust values, what little it does show being quite the reverse-namely, a maximum of clear weather in the middle of the day and a minimum at night. This clearly indicates that when the dust layer falls below the summit at night, radiation at once forms an independent cap on the hill-top; and again in the afternoon, although the dust stratum envelopes the summit, the opposite radiation warms it up and prevents condensation, or rather evaporates the watery particles of the cloud. So that, contrary to public opinion, the best time to visit the summit for the sake of the "view" is the middle of the day, and not the early morning. During fine settled weather the rise and fall of this cloud stratum can be followed, but in average weather the effect of radiation completely masks it. The effect of solar radiation and nocturnal radiation on dust, as particles and as strata, is a problem that has to be studied and worked out. Very little is definitely known about it at present.

In the study of the nature and motions of clouds the dust observations will be of great value. When a fog envelopes the summit, the number of dust particles observed may vary greatly without any apparent change in the thickness of the fog, but as a rule dry thick fog contains a great amount of dust, while thin wet mist contains very little. It is when a thin drizzling mist envelopes the summit that the lowest values are always obtained, and then there is a distinct difference between the conditions at sea-level and those at the summit, the winds at the latter place differing in direction by 90° or more from the winds below, and sometimes the upper winds are blowing straight out from the centre of a shallow low-pressure area, and the dust that rises with the slight ascending currents of the lower strata is almost entirely filtered out before reaching a height of 4400 feet. One of Mr. Aitken's conclusions may briefly be put as follows: Much wind, little dust; much dust, little wind. That dust seems to accumulate in the quietest places is fully borne out by the Ben Nevis observations. This is true not only horizontally, but also vertically, and it seems probable that this is what chiefly determines the position of cloud strata at all heights. And from this we may infer that the motion of clouds is much slower than that of the general aërial currents; and again, since clouds tend to form between currents, and may have as direction of motion the resultant of the directions of these currents, it follows that as indices to the motions of the upper air the velocity and motion of clouds are very unsatisfactory.

Observations of the apparent haziness of the atmosphere are made whenever it is possible, and the relations between the haziness of the air, the humidity, and the number of dust particles, have been found to be the same as what Mr. Aitken pointed out. Briefly, he found that with a constant humidity the haziness increased or diminished with the number of dust particles, and with a constant number of dust particles the haziness depended on the humidity (at least when the air was within 10 or 15 per cent. of saturation); for with increase of humidity the air became thicker, because apparently condensation begins on the dust particles before the air reaches its point of saturation.

The dust observations promise to be of special value in the study of weather types. In some weather types, not only are the dust values very abnormal, but the daily variation is in some instances quite abnormal also, indicating that the cloud or dust strata are differently situated from what they are in average weather, and also that their daily rise and fall occur at different times. In March 1890, the dust values show this very well below are the three-hourly means for each of three different periods :

First Period (12 days).

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Number per cubic centimetre . .

78

Prof. Judd, who has kindly sent me a copy, I extract the following:

Pantelleria, an island (13'5 by 8 kilometres), situated between Sicily and Tunis, is entirely of volcanic origin.1 The volcanic activity would at present appear to be a shade less marked than in the "Phlegræan Fields," west of Naples.

In Pantelleria we have exhalations of CO2; hot springs (of which those at the lake called "Bagno del Acqua," among other things are, we are told, so rich in alkalies as to lather, and be used for washing clothes !), and fumaroles, some of which exhale steam harmless to vegetation, and with little if any specific effect on the rocks, while others give out sulphurous vapours at 88° C. or more, 102 decomposing the rocks about them.

22

61 78 67 113 408 258
Second Period (3 days).
2867 1785 917 4733 4213 4295 3417 2533
Third Period (5 days).

65 25 37 19 20 28 93 76
During the third period of five days the weather was
very remarkable.
A large depression was slowly pro-
gressing eastwards to the north of Scotland, and the
winds on Ben Nevis were blowing almost straight out
from the centre, while the winds at sea-level were circu-
lating in the normal direction. This is the usual type
when low dust values are obtained; but it is difficult to
quite account for the daily variation in the dust values
being reversed, the higher values occurring at night, and
the lower in the middle of the day. This and many other
points have not been studied yet.

Dr. Buchan, in his recently published work on "Atmospheric Circulation," hinges his explanations of various atmospheric phenomena on the effect of solar and nocturnal radiation on the dust in the atmosphere, and accounts it one of the most important factors in the study of modern meteorology. The observations made at Ben Nevis Observatory clearly show that for observing the number of dust particles in the air, with a view to the observations being applied to the study of atmospheric phenomena, a true peak is of all places the best, because we can study not only the horizontal distribution of dust as brought by the different winds, but also, to a certain extent, the vertical distribution by the ascending and descending motions of the air past the place of obserANGUS RANKIN.

vation.

OF

ABSTRACT OF MR. A. RICCO'S ACCOUNT OF THE SUBMARINE ERUPTION NORTHWEST OF PANTELLERIA, OCTOBER 1891.1 F what happens in submarine eruptions we naturally know little. The evidence of Graham's Island (1831)2 and the eruption off Pantelleria (1891), to the south of Sicily, and of the damaged telegraph cables and various surface phenomena 3 to the north, towards the Lipari Isles, shows us that such eruptions are not rare in the Sicilian district, and any records of these fleeting occurrences that we can get, in the way of observation and specimens, may well prove of increasing interest as others are obtained to compare with them.

Mr. A. Ricco has recently published a detailed and illustrated account of the facts he was able to gather, concerning last October's submarine eruption north-west of Pantelleria, either in person or from local and other observers, he having reached the island during the latter part of the eruption. From this, at the suggestion of 1 Annali dell' Ufficio centrale Meteorologico e Geodinamico, ser. ii., Parte 3, vol. xi.

2(a) Lyell's "Principles of Geology"; and (b), for Bibliography, Johnston-Lavis's "South Italian Volcanoes," pp. 105-107.

3(a) South Italian Volcanoes," pp. 64 and 65; and (6) Giov. Platania, "I Fenomeni Sottomarini durante l'Eruzione di Vulcano (Eolie) nel 18881889," Att. Rend. Acc. Sc. Let. Art. Acireale, n. ser., vol. i., 1889, pp. 16, tables 3.

There is but doubtful record of seismic disturbances in earthquakes occurred, with elevation of part of the north the island prior to the summer of 1890. Then, however, coast, the cracking of cisterns, and an increase in the number and activity of the fumaroles, so that vineyards formed in some of the old craters were damaged. October 14, 1891 (three days before the eruption). These more than a year's interval, earthquakes again commenced apparently a further rise on the north coast, with surface were accompanied by drying up of certain springs, and

cracks in that district.

After

As the shocks were most violent and vertical at the

little town of Pantelleria itself (at the end of the island nearest the scene of eruption), they caused considerable consternation; and if one went by the account of the overstrung inhabitants, who felt shocks not recognized by the seismoscopes, one might exaggerate their violence. On the other hand, the walls of the houses, which outside the town have frequently no upper story, are, on the whole, substantially built, so that the insignificant damage (Fig. 1) appears to have been raised, in the two years, done is perhaps hardly a gauge. Part of the north coast

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FIG. 1.-Map of Pantelleria, showing the position, according to Ricco, of (a)
the submarine eruption of October 1891, and (, ) of the raised coast.
some 80 cm., the old sea-level being marked by a line of
white incrustations; and we are told that, according to
a recent estimate, the tide in this part of the Mediterra-
nean has an amplitude of but some 8 cm. ; besides, there
was the evidence of inhabitants who had bathed, boated,
and fished along the coast. The submarine eruption
(4 kilometres north-west of the island, Fig. 1) began on
Foerstner, "Nota preliminare sulla Geologia dell' Isola di Pantelleria"
(with geological map), Boll. Com. Geol. d'Ital., 1881.
Prof. G. Grablovitz, Le isorachie della marea nel Mediterraneo,"
Rendiconti della R. Accad. dei Lincei, 16 Agosto, 1891.

October 17, 1891, when the earthquakes abated, and water returned to some of the wells. The appearance of the sea, as viewed from the land, at first suggested the presence of some "great fish," and columns of "smoke" were seen. Those who visited the spot later (Fig. 2) found black

IG. 2.-Part of a sketch of the submarine eruption near Pantelleria, October 1891. (After Ricco.)

scoriaceous bombs rising to the surface, along a line some kilometre in length, extending north-east and south-west, which might well indicate a submarine fissure, the activity being specially great at certain points. Some of the bombs discharging steam ran hissing over the water with the recoil. Many were still very hot inside, fusing zinc (415 C.), and one was red-hot (in daylight), but below 800 C.. Some pieces were thrown 20 m. in the air, as I gather, not so much by their momentum on reaching the surface as by the explosions occurring there. After the explosions the fragments sank, the material having a sp. gr. of about 2'4. The highest temperature of the water obtained was but 1° C. above that of the surrounding sea. Ricco now questions the trustworthiness of the soundings made at the scene of eruption to a depth of 350 m. without feeling bottom, and he was told that fishermen had previously found but 160 m. of water there. Though some saw bubbles rise to the surface, the gases usually emitted in the case of subaerial eruptions were not detected in the sample of water collected, which Riccò suggests may be due to their having been taken into solution by the water lower down. However, there was a smell" as of gunpowder " at the spot; and the dark, basic, spongy matter of the bombs (previously described), "the only solid material erupted," gives out when heated a sulphurous odour, a fact of which Mr. F. Chapman had previously informed me. The eruption terminated on October 25, and the erupted matter disappeared.

Europe, and an exorbitant price is naturally asked for it. In South Africa the Giraffe is practically extinct, being only still met with in a few isolated localities nearly a thousand miles from Cape Town. In East Africa there are still Giraffes, and in places nearer the sea-board; but here, apparently, there are no means of catching them alive, as the natives do not understand how to do it. Here, however, it is that there appears to be most like lihood of obtaining a fresh supply. This will be an expensive business, but unless some steps are soon taken in the matter it seems that the younger generation of England will grow up without knowing what a living Giraffe is like. Their parents have been more fortunate. From the list given below, it will be seen that there have been 30 individuals of the Giraffe exhibited in the Zoological Society's Gardens since 1836, of which 17 have been born there, and 13 acquired by purchase. Of these 30, one was presented to the Royal Zoological Society of Ireland in 1844, five have been sold at prices varying from £450 to £150, and the remainder have died in the Gardens.

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I should add, in conclusion, that I have ascertained from Dr. Errera, who has charge of the seismological apparatus on the island, that the telegrams published in an English daily paper, as to renewed eruptions in the neighbourhood at a later date, were quite without founda- 30, 8

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29

Sold Oct. 29, 1853.

Born in the Menagerie, March,, March 29, 1853.

Died May 21, 1872.

Νον. 6, 1866.
Dec. 2, 1859.

Sold May 1, 1863.
Died Dec. 18, 1861.

Nov. 18, 1863.
April 21, 1864.

Mar. 31, 1865. April 3, 1865. April 20, 1865. Sold May 31, 1866. Sept. 14, 1866. Died Nov. 6, 1866. Mar. 17, 1867.

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June 20, 1881.

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Sept. 12, 1869.

April 27, 1874. May 21, 1878. Jan. 8, 1879. July 9, 1886. Nov. 24, 1891. March 22, 1892.1

GIRAFFES.

THE Zoological Society of London, as our readers, know, have lost their last remaining Giraffe, and, for the first time since 1836, no example of this, one of the most wonderful of living Mammals, is to be seen in the Regent's Park Gardens. Nor does it seem likely that the loss can be easily restored. At the present time, owing to the Mahdists having closed the Soudan to trade, the Giraffe market is very poorly supplied. Only one specimen of this animal, we are told, is for sale in NATURE, vol. xlv p. 251.

NOTES.

THE ordinary general meeting of the Institution of Mechanical Engineers will be held on Thursday evening, May 5, and Friday

The President

evening, May 6, at 25 Great George Street, Westminster, by chair will be taken at half-past seven p m. on each evening, by the President, Dr. William Anderson, F. R. S. will deliver his inaugural address on Thursday evening, after which the following papers will be read and discussed, as far as time permits :-Research Committee on Marine-Engine Trials : Report upon trial of the steamer Ville de Douvres, by Prof. Alexander L. W. Kennedy, F.R.S., Chairman (Thursday, and discussion continued on Friday). On condensation in steam

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