Calibrate Spectroscope to Find Wavelength

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SUMMARY

The discussion centers on calibrating a spectroscope using known emission wavelengths of 425nm, 565nm, 600nm, and 700nm, which correspond to measured positions of 32mm, 59mm, 63mm, and 69mm, respectively. The student seeks to determine the wavelength of an emission line at 55mm using the equation dsin(θ) = m(λ). Key challenges include the lack of information on the diffraction grating spacing and the angle θ. Participants emphasize the importance of understanding the spectroscope's mechanics and suggest assuming m=1 to simplify calculations.

PREREQUISITES
  • Understanding of diffraction and the equation dsin(θ) = m(λ)
  • Familiarity with spectroscope operation and calibration techniques
  • Basic knowledge of graphing and using Excel for data analysis
  • Concept of fringe spacing and its relation to wavelength measurements
NEXT STEPS
  • Research the mechanics of spectroscopes and how they measure wavelengths
  • Learn how to derive and apply the equation dsin(θ) = m(λ) in practical scenarios
  • Explore methods for determining the order "m" of emission lines in spectroscopy
  • Practice using Excel to plot data and generate equations of lines for calibration
USEFUL FOR

Students in physics or engineering, educators teaching optics, and anyone involved in experimental spectroscopy who seeks to understand spectroscope calibration and data interpretation.

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Homework Statement


A student collects diffraction data using a lamp with known emission wavelengths of 425nm, 565nm, 600nm, and 700nm. These lines appeared on her spectroscope at 32mm, 59mm, 63mm, and 69mm(all measured from the same arbitrary 0mm position). With these data she is able to calibrate her spectroscope, and using this calibrated spectroscope she observes another lamp that has an emission line at 55mm. What is the wavelength of this emission line? (Use Excel to generate an equation of a line with a properly labeled graph)

Homework Equations



dsin(θ) = m (λ)

The Attempt at a Solution



In the equation above, I am provided with two out of four variables - I don't have the diffraction grating difference, nor do I have the angle at each wavelength.

What I thought is this: sin(theta) = x (spacing between bright fringes, i.e 32mm) / L (path length). If I substitute it into the equation above, I would get dx / L = m (λ). I still am missing two variables. Even if I had tan(θ) = x(fringe spacing) / L, and I assumed sin(θ) ~ tan(θ) as the angle is small, I'm still utterly confused. Now I attempt to address the last part of the problem in parentheses - plotting the equation - I had thought that in mλ = dsinθ, I would be able to find the slope to be some variable, but it seems I am still at a disadvantage without more information in the problem.

Any tips? I'd appreciate anything - better just tips rather than the whole solution if possible; I still want to try and arrive at the solution myself.
 
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Would it help if you knew the order "m" of the emission line(s)?
I think you need a sketch of how the spectroscope works: how do you get from ##d\sin\theta = m\lambda## to "mm from some arbitrary 0mm position"?
 
Simon Bridge said:
Would it help if you knew the order "m" of the emission line(s)?
I think you need a sketch of how the spectroscope works: how do you get from ##d\sin\theta = m\lambda## to "mm from some arbitrary 0mm position"?
I think I'm supposed to assume that m is 1 and each wavelength is related to each fringe spacing provided...unsure because the text above is all the professor provided.

I'll try looking up how the spectroscope works; but I believe the mm values given are x, or the fringe spacing - measured from the central maximum - perhaps the central maximum is the "0mm?"
 
The text says that the 0mm position is "arbitrary" - therefore you cannot assume the position is from the central max.
Another thing to wonder about is if the spectroscope works so that the angle ##\theta## is small...

Bottom line: the data is useless unless you know how the spectroscope works ... ie. there could be a lens in it.
So you will have to check your notes to see what sort of thing is expected.

If you decide that the spectrscope data is consistent so that m is the same between reading, or that m=1 every time, then you have eliminated a variable. But the question was: does it help?

One of the ways to reduce the number of variables is to compare results between trials ... like if you look for ratios?
 

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