What is the wavelength of the x-rays in the direct beam?

AI Thread Summary
The discussion centers on determining the wavelength of x-rays in a direct beam after scattering from a target. The Compton effect formula is applied, where the scattered wavelength is given, but the target's identity is deemed irrelevant for calculations. The Compton wavelength, which is a constant derived from fundamental constants, does not depend on the target material. It is clarified that the x-rays interact with electrons in the target, leading to scattering and a recoiling electron. Understanding the conservation of energy and momentum in this context is essential for grasping the Compton effect.
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for the following question:
a beam of x-rays is scattered b a target. At 45 degrees from the beam derection the scattered x-rays have a wavelength of 2.2pm. What is the wavelength of the x-rays in the direct beam?

my problem:
the question doesn't specify what the target is...
so what are you supposed to plug in for the compton's wavelength if you the compton effect formula?
 
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Don't you just use the expression:

\lambda-\lambda_0 = (h/m_ec)*(1-cos(\theta))

Where \lambda is the scattered wavelength and \lambda_0 is the original wavelength. The term h/m_ec is the comptom wavelength and you can just check that value in your book no doubt. So the target source is irrelevant for this problem (I think).
 
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for the term, h/m_ec,
doesn't m depend on the target?
 
Nope it doesn't depend on the material at all. h is Planck's constant, c is the speed of light and m_e is the mass of the electron, which are all independent of the target material. You can calculate its value based on that information, or you can look in your book and it should give an accepted value for the compton wavelength (h/m_ec).
 
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i think i don't get the formula thoroughly... i thought the x-rays were supposed to hit the target, and get scattered by it~
unless the target is the electron, why's m_e the mass of the electron?
 
Okay you have your x-rays which are incident on a target source. The incident x-rays have a wavelength \lambda_0. Now what happens is that the x-ray is scattered from an electron in the target source. The scattered x-ray has a new wavelength \lambda'. Now in this process there is also a recoiling electron, which has the compton wavelength \lambda_c = h/m_ec
 
so it doesn't matter what the target is...
whatever target the photon hits will send off an electron?
 
Yeah if the photon does interact with the target source there will always be a recoiling electron in order to be consistent with the fact that energy and momentum are conserved.
 
i understand it a whole better~
thank you very much for explaining! :)
 
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