
Principles of DIC Microscopy
since the human eye, cameras, and film caprure images by recording differences in light intensity and cotor,
they do not register colorless, transparent cells or baCreria. Although dyes can be used to make these
transparent subjects visible' the dye itself kills them. The differentiàt inteterence "onira.i iòio*i,ni"ro""op"
was deveroped in order to permit the observation of transparent subiects whire they are .tii "ìiul.
The basic structure of the Drc microscope is the same as that of an ordinary microscope, except that it
includes polarizing plates and wollasîon prisms'. inese ffiat erements change a transparent subject into
different levers of right inlensity. In other words, wnen yoLr ioot inrough a Drc microscope, you see even
]!Tqlt:tt tYb.,."cts as jmages consisting of different rivets of tighr inìtensity. 1-ruomaÀiibíi"iJ-"r" "rro
used as a variation of Wollaston prisms.)
The principles of a DIC microscope are discussed below
Light refracts as it passes through a subject, even if it is a colorless, transparent subiect. lf the refractive
index of a subject is ditferent Írom that of.its surroundings, light thar passes through the subject will reach a
ceiain destination point faster (or sloweo than light thaipaéés through the sunounding material. In short,
when lighî passes through a subject, it undergoei a pnaée cnanje lwitn me pnase eitÀJ, jJffi an"aa o,
being delayed).
A subjecl whose only effect on light is a phase change is
called a "phase subject." See Figure g-l on the rightl A
wavefront of light that is originalty in the same phise.
indicated by a single straight line, changes when it passes
through a phase subiect, so that onty th; light lhat passed
through the subject traveled faster than thelight that did not.
This phase change happens when light passés through a
mtcrosoope specimen, with the light passing through the
specimen traveling either faster or slower than the-
surrounding light.
Now look at Figure 3-2. This diagram illustrates the
principles.of a DIC microscope. In the diagram, the light
source is located on the left, so the light travels from Éft to
right. A polarizing plate and a Wollasion prism are each
placed on the condenser side and the obiective side.
When the light from the light source passes through
pol3îiilS plate 1 (th€ potarizeo, il wiil be potaize-cr (changed
to light that vibrates in one direction onty). When thià
polaized light passes through Wo aston prism f , it is sptit
into two rays that have mutually perpendicular planes oi
polarization (direction of vibration); the two rays travel at a
slighl distance from each other.
Polarlzing plate 1
Figure 3-2 Principles of a DIC microscope
since wollaston prism 1 is on the front focal plane of the condenser, the two rays pass through the specimen
in pafallel, at a slight distance from each other. The distance between the rays is called the ,shear." since
the shear is set berow the resorving power of the ob,ectivé, tne specimen does not appear as a doubre
rmage.
lftel,tlte lwo rays pass through the specimen, they are collected by the obiecîive onto the back focat ptane of
the obiective. wollaston prism 2 is placed here toiecombine tnà two rays 'uacr ino on".- Àorràu"r, the rays
do not intefere w*h each other since they have p€rpendicutariLnes ot poraization.
l9111zjno plate 2 (the analyzer) is placed so that th€ direction of potarization is perpendicutar to that of
polarizing plate I , taking out opposite phase planes in tne tight. where the speòiméÀ oio noì"i"ng" tn"
phas.e of the.light,.the two light rays intelere with """h otn"i, ,""r.ening them and m"iinf tno.à "r"". m rn"
vi€xffi€ld dark' where phase obiects-in the specimen cnangóo the phase of the righî, the two right rays oo
not interfere with each other, so those areas in the viewfield'appeai urignt. rnis oiieiencein urightness is
how the DIC microscope makes phase objects visible.
WavofÌont aft€r passlng
through spocimen
\
I
(
Wavgfroflt SD€cimen
>l
nl
Yal
lt
l subjecl
Pfrase
Figure 3-l Phase changas
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