Lenses and Waves
Lenses and Waves
Lenses and Waves
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142 CHAPTER 4<br />
it clear what kind of problem strange refraction constituted<br />
for the wave theory (Figure 46). It shows the strange<br />
refraction of a perpendicular ray along with, what seems to<br />
be, the propagation of waves. 126 After having passed the<br />
refracting surface, the waves proceed obliquely to their<br />
direction of propagation, which contradicts the assumptions<br />
of Pardies' theory. Thus this tiny sketch illustrates what<br />
Huygens called the ‘difficulté’ of strange refraction.<br />
Strange refraction posed a problem for the explanation of<br />
ordinary refraction that Huygens intended to adopt <strong>and</strong> he<br />
first wanted to solve it. His first attempt is recorded in those<br />
ten notebook pages. The notes are revealing. Despite the fact<br />
that strange refraction was a problem of waves, this tiny<br />
sketch is the only place where waves enter his investigation.<br />
Instead, Huygens approached strange refraction in a rather traditional way.<br />
He tried to find out what mathematical regularities rays refracted in Icel<strong>and</strong><br />
crystal might display. This was the same way Bartholinus had approached the<br />
phenomenon, namely by trying to find a law describing the behavior of<br />
strangely refracted rays.<br />
4.2.1 BARTHOLINUS AND HUYGENS ON ICELAND CRYSTAL<br />
Huygens began by recording the<br />
main characteristics of the crystal<br />
(Figure 47). 127 With explicit<br />
reference, he reproduced the<br />
crystallographic data of<br />
Bartholinus. The crystal has the<br />
form of a parallelepiped, of which<br />
the obtuse angles of each<br />
parallelogram like ACB are 101.<br />
Consequently, the angle AXB<br />
between faces GOCA <strong>and</strong> FOCB is<br />
10340' <strong>and</strong> those between lines<br />
OC <strong>and</strong> CI (bisecting angle BCA) is<br />
Figure 46<br />
<strong>Waves</strong> through<br />
the crystal.<br />
7234'. A ray of light falling on a<br />
Figure 47 Shape <strong>and</strong> main angles of the crystal.<br />
face of the crystal is double<br />
refracted. One of the refractions conforms to the sine law, whereby the<br />
index of refraction is approximately 5 to 3, a value Bartholinus had<br />
determined empirically. The other refraction does not follow the sine law<br />
<strong>and</strong> is therefor called extraordinary or strange. Huygens observed some<br />
physical characteristics of the crystal as well, in particular the fact that the<br />
126 I experienced some difficulty seeing this sketch as a two-dimensional section, as most historians have<br />
done. I once thought it was meant to be drawn in perspective, a ray refracted out of the paper towards the<br />
reader. Despite this ambivalence, I think after all that the two-dimensional interpretation is correct.<br />
127 Hug2, 173v <strong>and</strong> 175r. OC19, 407-408; Bartholinus, Experimenta, 8-11 <strong>and</strong> 40.