The Glaciers of the Alps: Being a narrative of excursions and ascents, an account of the origin and phenomena of glaciers and an exposition of the physical principles to which they are relatedTyndall, John
Science
The Glaciers of the Alps: Being a narrative of excursions and ascents, an account of the origin and phenomena of glaciers and an exposition of the physical principles to which they are related
Tyndall, John
Alps -- Description and travel; Glaciers -- Alps
Description, however, can give but a feeble idea of
these exquisite effects;--
"Thou canst not wave thy staff in the air,
Or dip thy paddle in the lake,
But it carves the brow of beauty there,
And the ripples in rhymes the oar forsake."
[Sidenote: CHASING PRODUCED BY WAVES.]
[Illustration: Fig. 16. Chasing produced by waves.]
[Sidenote: EFFECT OF RETARDATION.]
Now, all that we have said regarding the retardation of the waves of
water, by a whole undulation and a semi-undulation, is perfectly
applicable to the case of light. Two luminous points may be placed near
to each other so as to resemble the two stones dropped into the water;
and when the light of these is properly received upon a screen, or
directly upon the retina, we find that at some places the action of the
rays upon each other produces darkness, and at others augmented light.
The former places are those where the rays emitted from one point are an
_odd_ number of semi-undulations in advance of the rays sent from the
other; the latter places are those where the difference of path
described by the rays is either nothing, or an _even_ number of
semi-undulations. Supposing _a_ and _b_ (Fig. 17) to be two such
sources of light, and S R a screen on which the light falls; at a point
_l_, equally distant from _a_ and _b_, we have _light_; at a point _d_,
where _a d_ is half an undulation longer than _b d_, we have darkness;
at _l'_, where _a l'_ is a whole wave-length, or two semi-undulations,
longer than _b l'_, we again have light; and at a point _d'_, where the
difference is three semi-undulations, we have darkness; and thus we
obtain a series of bright and dark spaces as we recede laterally from
the central point _l_.
[Illustration: Fig. 17. Diagram explanatory of Interference.]
Let a bit of tin foil be closely pasted upon a piece of glass, and the
edge of a penknife drawn across the foil so as to produce a slit.
Looking through this slit at a small and distant light, we find the
light spread out in a direction at right angles to the slit, and if the
light looked at be _monochromatic_, that is, composed of a single
colour, we shall have a series of bright and dark bars corresponding to
the points at which the rays from the different points of the slit
alternately coincide and interfere upon the retina. By properly
drawing a knife across a sheet of letter-paper a suitable slit may also
be obtained; and those practised in such things can obtain the effect by
looking through their fingers or their eyelashes.
[Illustration: INTERFERENCE SPECTRA, PRODUCED BY DIFFRACTION.
Fig. 18. _To face_ p. 235.]
[Sidenote: CHROMATIC EFFECTS.]
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