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its bathing medium), there will be very little difference in amplitude<br />

between the light which passes though the medium and that<br />

which passes through the specimen. There will, however, be a<br />

phase difference introduced because of the refractive index difference<br />

between the medium and specimen. Because the eye cannot<br />

detect differences in phase, the purpose of the interference microscope<br />

is to convert the phase difference into an amplitude difference.<br />

One way of doing this is to use round-the-square interference<br />

(fig. 21.9).<br />

Comparison slide<br />

M] I () t () ~S1<br />

Light sourse x { , ]I ~ y<br />

SI<br />

~ Eye<br />

Fig. 21.9. The interference microscope (see text for explanation)<br />

o B 0 c<br />

I<br />

Fig. 21. 10. Vector representation of background and transmitted light:<br />

a ­ the vector DB represents the background light and OT the light<br />

transmitted through the object; b ­ DC represents the amplitude and<br />

phase of the light which has passed through the comparison slide; c ­<br />

the phase of DC has been adjusted so that it is exactly out of phase<br />

with light transmitted through the object OT; d - the background<br />

does not appear dark as the background vector DB and comparison<br />

vector DC are not 180 0 out of phase<br />

148<br />

~ c~~~~_ ~ R~.<br />

T 0 B 0 0 B<br />

a b c d u<br />

/,<br />

'1;<br />

I<br />

I<br />

b<br />

microscope<br />

Lb<br />

Fig. 21.12. Mechanism of diffraction of light by a narrow slit<br />

of width a: a ­ condition of maximum; b ­ condition of minimum<br />

149<br />

a<br />

The observed image arises<br />

from the sum of two light<br />

beams. One passes though the<br />

object and the other traverses a<br />

comparison slide in a manner<br />

by which the phase and amplitude<br />

of the comparison beam<br />

can be adjusted. In fig. 21.10<br />

the vector OB represents the<br />

background light and OT the<br />

light transmitted through the<br />

object. As the latter has a slightly higher refractive index than the<br />

suspending medium, OT will be directed behind OB by a small<br />

angle (fJ). The phase of the light passing through the comparison<br />

slide is now adjusted so that it is exactly out of phase with light<br />

transmitted through the object. Contrast is therefore achieved and<br />

the object appears dark in a bright surround (fig. 21.11).<br />

21.3.5. Diffraction<br />

Diffraction is the apparent bending of light waves around<br />

obstacles in its path. Bending is due to Huygen's principle, which<br />

states that all points along a wave front act as if they were point<br />

sources. Thus, when a wave comes against a barrier with a small<br />

opening, all but one of the effective point sources is blocked. The<br />

b<br />

",.l('l bsin8 = (2m +1) )../2<br />

...<br />

b

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