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Lecture
1 II| the way in which we use a ray of light for the purpose 2 II| possesses of attracting a ray of light. If Mr. Anderson 3 II| spectrum on the screen]. This ray of light is bent out of 4 II| mica. Here, you see, is our ray of light: we have first 5 II| then, we have our polarized ray of light, and I can so adjust 6 II| nothing in the course of this ray of light but what is perfectly 7 II| glass into the polarized ray so as to show you that it 8 II| Here, then, we have our ray of polarized light, and 9 II| the path of the polarized ray, I believe it will do nothing. 10 II| again placed across the ray of light.] Now you see how