- #1
doofus
- 5
- 0
I am playing with a basic prism spectrometer for fun, and because a lot of design about these spectrometers has gone to the void over the years. As simple as this system is, my optics knowledge is ancient, and I have, unexpectedly encountered a puzzle. The set up is the following:
Linear path:
White LED -> 2mm tall x 100um wide slit -> planoconvex collimating lens (60mm focal length) -> Equilateral triangular glass Prism with a circumradius of ~2.5cm.
The incident angle of the collimated beam is roughly 70 degrees from normal on one of the prism faces.
The light refracts through the prism, thanks Snell, and if I follow its path with an index card I see a spectrum of colors emerge out the other face. I understand that on the screen what I am seeing is the overlap of the collimated beam at many wavelengths slightly offset from one another in space, but never the less each wavelength is overlapping with those nearby it.
Now what I've been told, in many old textbooks, is if I place a lens in the path of these refracted beams I will be able to image the diffraction slit, but the superposition of all of the wavelengths will remain spatially separated. Meaning I will obtain a spectrogram, which has less overlap of light intensity from the refracted beams.
In practice I do not obtain this result. As I move my screen from the lens to it's focal point I watch the rainbow of colors collapse into an image of the original slit? That is to say, there is no spectrogram, only white light in a shape and size which is highly similar to the original slit. As I go further from the focal point I again observe a rainbow image, but it grows out of focus. Why might I not see a "resolved" spectrogram in the focal plane? Is there a way to increase the horizontal size of the "resolved" spectrogram?
Linear path:
White LED -> 2mm tall x 100um wide slit -> planoconvex collimating lens (60mm focal length) -> Equilateral triangular glass Prism with a circumradius of ~2.5cm.
The incident angle of the collimated beam is roughly 70 degrees from normal on one of the prism faces.
The light refracts through the prism, thanks Snell, and if I follow its path with an index card I see a spectrum of colors emerge out the other face. I understand that on the screen what I am seeing is the overlap of the collimated beam at many wavelengths slightly offset from one another in space, but never the less each wavelength is overlapping with those nearby it.
Now what I've been told, in many old textbooks, is if I place a lens in the path of these refracted beams I will be able to image the diffraction slit, but the superposition of all of the wavelengths will remain spatially separated. Meaning I will obtain a spectrogram, which has less overlap of light intensity from the refracted beams.
In practice I do not obtain this result. As I move my screen from the lens to it's focal point I watch the rainbow of colors collapse into an image of the original slit? That is to say, there is no spectrogram, only white light in a shape and size which is highly similar to the original slit. As I go further from the focal point I again observe a rainbow image, but it grows out of focus. Why might I not see a "resolved" spectrogram in the focal plane? Is there a way to increase the horizontal size of the "resolved" spectrogram?