CHAPTER III

CIRRO-STRATUS AND CIRRO-CUMULUS

SEVERAL of the varieties of cirrus already discussed may gather so

abundantly at some given level in the atmosphere, that the most obvious

feature comes to be this arrangement in a sheet. The cloud then

becomes cirro-stratus, and should be so named. We have described how

cirro-nebula frequently grows in density until it fails to produce halo

phenomena, and may even reduce the sun to a hazy patch of light showing

no outline. This is the most typical of all forms of cirro-stratus.

It has always a distinctly fibrous or streaky appearance, whereby it

is at once distinguished from a similar but lower cloud which will be

described later on.

A similar sheet may be formed from the fusion together of the streaks

of cirrus-nebulosus, the bands of cirrus vittatus, or the development

of cirrus inconstans. But the general rule is that the cirro-stratus

retains more or less of the specific characters of the parent form.

Plate 14 shows a hazy form of cirro-stratus developed from the nebulous

cirrus. Its altitude was great, being about 10,000 metres. The

processes of growth and change could be studied easily. First would

appear some faint spots and streaks; these quickly fused together

into larger patches, which again joined to their neighbours. In a few

minutes the cloud so formed would return to the mottled or streaky

appearance, and either disappear entirely or become very thin, only

to recommence the process. This went on for more than an hour, the

cloudy patches getting larger and larger, until the critical condition

was passed, and the sky was covered with a general veil of typical

cirro-stratus.

[Illustration: Plate 14.

HAZY CIRRO-STRATUS.

(_Cirro-stratus Nebulosus._)]

In Plate 15 we have an example of a cloud which is clearly

cirro-stratus, but the sheet is broken up into long bands, and each of

these is made up of common cirrus. In the upper part of the picture

the sprays of cirrus are forming, and as they come into being they

are arranged in rows. We have here to do with a phenomenon of a very

different order from the one presented by the true banded cirrus. The

arrangement into belts must here be due to some kind of wave-movement

in the air, breaking up the critical plane into long ribs transverse

to the direction of the wave-movement. The specimen shown was moving

in a direction nearly at right angles to the bands, though the surface

wind was nearly parallel to their length. The question at once

presented itself as to whether the movement of the bands was really a

drift of the cloud, or whether it was not a case of the propagation

of cloud production with the advancing wave. This was easily answered

by watching the details of a band. The advancing side was always

feathery, and careful observation showed that the edge advanced by

throwing out new threads and curls. A given thread or curl, one moment

at the edge, would in a few minutes be well in the band. Quite opposite

events were taking place in the rear of each band. The cloud was there

obviously melting away. Indeed, to sum the matter up, the cloud bands

flowed past their details just as the waves on the sea flow past the

floating foam. Evidently we have in Plate 15 the result of a plane of

commencing cirrus formation broken into a series of troughs and waves

by an undulatory movement of the air. But, as we have already said

when speaking of cirrus inconstans, the condition in which trifling

up-and-down movements can determine whether condensation shall, or

shall not, take place seldom lasts long. It is usually only a stage

in a continuous change, and in this particular instance the banded

structure was soon replaced by a fairly continuous sheet of typical

cirro-stratus.

[Illustration: Plate 15.

CIRRO-STRATUS.]

The next plate, No. 16, shows a similar process. In the upper part we

have cirrus inconstans forming in patches out of a deep clear-blue sky.

Its hazy fibres grow closer and closer, betraying a slight tendency to

gather in narrow ripple-like bands, but the structure is soon lost in

the uniform white sheet of interlacing fibres, which differ from common

cirrus in little else than their number and closeness. Nevertheless,

the stratiform arrangement is quite obvious enough to warrant the use

of the term “cirro-stratus.”

[Illustration: Plate 16.

CIRRO-STRATUS.

(_Cirro-stratus Communis._)]

The change of cirro-nebula into cirro-stratus is shown in Plate 4, to

which reference has already been made. The structures are remarkably

delicate, showing in the middle a distinct irregular mottling; and

rather further towards the top right-hand corner a ripple structure

appears, and in the top left-hand corner the sheet is denser and

whiter. The altitude of this cloud was evidently great, and actual

measurement showed it to be 7·6 miles. It did not last long, and after

its change into broken patches of denser cirro-stratus, still higher

clouds were revealed through the gaps.

Cirro-stratus often forms almost simultaneously at more than one level,

and when that happens the full stratiform appearance is generally

reached first by the lower layer. In Plate 17 we have two layers. The

fluffy bits of cirrus nebulosus, in the lower part of the picture, are

really the higher clouds. Below them, probably by many thousands of

feet, floats the denser cloud shown in the upper part of the picture.

This is an interesting link between the fibrous and the granular forms

of cirrus, and is probably best described as spotted cirro-stratus,

or cirro-stratus maculosus. It is a form very frequently met with,

but seldom showing any persistence. It is indicative of condensation

in a calm atmosphere, and not unfrequently marks either the small

irregularities of pressure which form the conditions for thunderstorms,

or the beginning of the break up of an anticyclone.

[Illustration: Plate 17.

FLOCCULENT CIRRO-STRATUS.

(_Cirro-stratus Cumulosus._)]

A coarser texture and greater density are shown in Plate 18, where we

have cirro-stratus in the lower part of the picture, and cirro-cumulus

in the upper. The altitude of this cloud was only about 4000 metres,

one of the least values recorded at Exeter for cirro-stratus of any

kind. The intimate admixture of the fibrous and granular forms is very

clearly shown.

[Illustration: Plate 18.

CIRRO-STRATUS AND CIRRO-CUMULUS.]

This close relation is equally obvious in Plate 19, where the cloudlets

are arranged in loosely marshalled rows, dimly resembling the banded

structure of Plate 15. But in this case the direction of movement was

with the long lines, and the propagation of cloud production followed

the same course. Some of the little cloudlets have an opacity, and

therefore brilliancy, quite unusual for cirro-cumulus, but their

intimate association evidently in the same plane with undoubted cirrus

shows that they must fall under that general description. It is a cloud

indicative of unsettled weather, and the exceptional brilliancy is

doubtless due to an unusual quantity of vapour at the cloud plane,

which must mean that the change from the dry stratum above to the damp

one below must be much more sudden than is ordinarily the case. Clouds

of this kind might well be called cirro-stratus cumulosus.

[Illustration: Plate 19.

CIRRO-CUMULUS.]

We now come to two companion pictures, Plates 20 and 21, which were

taken within half a minute of each other. In the first the camera

was directed towards the west, and in the second it was facing the

north-west. The sun was nearing the horizon, and was only just outside

the field of view in each case, so that the two photographs form

a panorama of the western sky. A solar halo had disappeared about

half an hour previously, and the cirro-nebula had changed into the

remarkable forms of cloud depicted. Plate 21 shows cirrus ripples in

the upper part, and cirro-cumulus in soft, ill-defined balls in the

lower part; but they were at the same level, and are only different

parts of the same cloud plane. In Plate 22 we see similar ball-like

cloudlets ranged in long lines which run almost at right angles to

the ripples of the companion picture. Clouds like these are rare.

They are almost unknown during the early part of the day, and, so

far as the writer’s experience goes, they are only to be found in

the afternoon towards sunset. Some of our most gorgeous sunset skies

are due to them; for their altitude is considerable, and they do not

light up with the sunset colours until the lower clouds have become

dark shadows against the glowing background. The hottest months of the

year, the still air and great evaporation which are the contributing

causes of thunderstorms, are also the conditions under which such

skies may be seen. Indeed, while these photographs were being taken,

heavy thunderstorms were in progress within less than a hundred miles.

Cirro-cumulus nebulosus, or hazy cirro-cumulus, describes the form

correctly.

[Illustration: Plate 20.

HAZY CIRRO-CUMULUS.

(_Cirro-cumulus Nebulosus._)]

[Illustration: Plate 21.

HAZY CIRRO-CUMULUS.

(_Cirro-cumulus Nebulosus._)]

The next plate, No. 22, gives a view of an evening sky about half an

hour after sunset. The lower clouds, cirro-cumulus and cirro-stratus,

of a deep purple brown, standing out dark against a gold-coloured sheet

of higher cirro-stratus, which comes out white in the photograph, while

the purple-tinted sky comes dark. We have here three distinct layers,

all cirrus. First, the hazy cirro-cumulus, forming two bars across the

lower part of the picture; then long bands of cirrus or cirro-stratus,

best seen in the bottom right-hand corner; and, far above both, the

cirro-stratus which was reflecting the yellow sunlight. Such a sky

might be an indication of thunder conditions, or it might be due to an

unusual quantity of vapour in the atmosphere produced by some other

cause. The actual conditions were the gentle flow over England of

vapour-laden air from the western ocean, heralding the change from a

long spell of fine hot weather, due to a July anticyclone, to a month

of heavy rains and western gales, accompanying the passage of a long

procession of cyclones along our western shores.

[Illustration: Plate 22.

A SUNSET SKY.]

Again, a marked contrast is shown in Plate 23. Here we have the highest

and thinnest form of cirro-cumulus, the one named cirro-macula by

Mr. Ley. It is rarely, if ever, seen before eleven o’clock in the

morning, and is far commoner in the afternoon. The example shown was

photographed at sunset at the close of a day which had been almost

cloudless. Cirro-macula forms here and there in a clear sky. A hazy,

whitish patch appears, which at first shows no definite structure, but

looks almost like a little bit of cirro-nebula. This suddenly splits

up by clear blue lanes running through it, and cutting the patch up

into irregular segments, which quickly round themselves off into minute

bits usually whiter on their edges and semi-transparent in the centre.

The process can be strikingly imitated by scattering on water some fine

powder which will float. If left without disturbance, the particles

draw together into numerous small groups, leaving lanes of clear water

between them.

[Illustration: Plate 23.

SPECKLE CLOUD (Ley).

(_Cirro-macula._)]

Cirro-macula frequently gives rise to the fibrous form of cirrus we

have called cirrus caudatus. The granules of the cirro-macula grow

denser, and begin to drop their frozen particles as soon as they become

large enough. Indeed, a cloudlet of cirro-macula may sometimes be seen

to turn bodily into a fine line of falling crystals, which will be a

curving line of cirrus. On the other hand, it will sometimes remain

visible for an hour or more without any trace of descending streaks or

floating fibres. Pure cirro-macula such as Plate 23 is not often seen;

it is far more frequently mixed with more solid-looking cloudlets and

descending fibres, such as are shown in Plate 24, which gives the same

point of view as 23, but a quarter of an hour later, and photographed

with a longer focus lens. These two photographs, together with 20 and

21, give excellent examples of the use of the black mirror. In none

of the four could the naked eye detect all of the cloud structures.

The whole sky was a blaze of dazzling light, but by adjusting exposure

and development the details are fully brought out without the least

difficulty.

[Illustration: Plate 24.

CIRRUS CAUDATUS AND CIRRO-MACULA.]

Cirro-stratus, we see from the examples which have been considered,

hardly deserves to be treated as a distinct genus of cloud. Its

formation is identical with that of many species of cirrus, or in some

cases with that of the speckle cloud, cirro-macula, or even the coarser

kinds of cirro-cumulus. The different varieties which it shows are best

rendered by reference to the specific names of the detached forms which

have similar features.

Cirro-cumulus, on the other hand, does present clearly marked

varieties. Cirro-macula is so distinct that it might well be given

the name awarded to it by Mr. Ley, while the term “cirro-cumulus” is

reserved for the coarser and rounder forms. The hazy, ripple-like

structures of Plate 4 and Plate 20 should also have some distinctive

appellation, as will be suggested later on when dealing with wave

clouds as a whole.

It is difficult to find any short way of expressing the various ideas

which should be summed up in the name of a cloud. There seems no

alternative to the use of additional words, unless it be to follow

the example of chemists, and compound appalling names similar to

those which terrify the uninitiated who think they would like to read

something about, let us say, the coal-tar dyes.

If a cloud belongs to the order cirrus, is in a level sheet, and

that sheet is composed of interlacing or curling fibres, like those

of common cirrus, we can hardly express the facts more briefly than

by calling it cirro-stratus communis, or common cirro-stratus. If

it consists of cirrus bands fused together, but still showing the

banded structure, it is cirro-stratus vittatus. Again, if it is finely

speckled, like cirro-macula, it may be described as cirro-stratus

maculosus, and if the structure is coarser it may be called

cirro-stratus cumulosus.

As a general average, cirro-stratus lies somewhat lower in the

atmosphere than the detached forms, probably because the conditions

which give rise to the latter reach to greater altitudes in patches

than it is possible for them to reach in a continuous manner. Vapour

becomes rarer with increased height and with diminished temperature,

so that it must, on the whole, be less frequently present in

cloud-producing quantity as the height increases. At great altitudes

it will be seldom that the quantity is great enough to produce a

stratiform cloud, though it may well be enough for cirro-macula, or the

detached forms of cirrus, like cirrus excelsus.

The production of cirro-cumulus and cirro-stratus sometimes spreads

across the sky with astonishing speed, and this rapid advance of the

edge of the cloud may lead to quite mistaken ideas as to the velocity

of the wind at that altitude. In the case of cirro-cumulus, or

cirro-macula, it is easy to fix attention on a single cloudlet. If this

has the usual ball-like form, it can only be regarded as floating in

the air and moving with it. Meanwhile new cloudlets may be forming and

growing denser, so that the cloud patch as a whole may be apparently

advancing at a much greater rate. Careless observation would then lead

to the idea that the cloud was moving much faster than it really is,

but if the attention is rigidly fixed on a particular cloudlet the

mistake is impossible. If the cloud is a variety of cirro-stratus,

it is not always easy, or even possible, to distinguish between the

advance of condensation and the movement of the whole, but it can

nearly always be done if the cloud shows any definite features upon

which attention can be fastened. Sometimes none sufficiently marked can

be seen, and when that happens it is still possible in most cases, by

watching the edge of the cloud-mass, to see whether new cloud is being

added to that edge. The wave-like forms present a special case, which

will be dealt with in a later chapter, after the general principles

of cloud formation have been discussed in connection with the great

clouds of the lower air, whose causes and conditions are far better

understood.

Cloud Studies · 第 3 / 11 章