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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.

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