Frequency to wavelength question (thermal Doppler broadening)

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The discussion centers on the relationship between frequency and wavelength, particularly in the context of thermal Doppler broadening. It clarifies that the equation \(\nu = c/\lambda\) does not directly apply to small variations in frequency and wavelength. The derivation shows that the product \(\omega\lambda\) remains constant, leading to the relationship \(\Delta\lambda/\lambda \simeq -\Delta\omega/\omega\). This highlights the importance of understanding variations rather than just the static relationship between frequency and wavelength. The clarification is essential for grasping the nuances of Doppler broadening effects.
dartingeyes
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Homework Statement
I don't understand how to go from one equation to the other
Relevant Equations
provided in picture
I want to understand how the two equations in the picture are the same. I am confused because \nu=c/\lambda. This would mean that the term on the right side of the equation in the square root, call it x, would then become x^-1. The resulting equation being \Delta\lambda = \lambda x^-1. But somehow this is not the case?
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What you are saying is only true for the relationship between frequency and wavelength themselves - not their small variation.

From ##\omega \propto 1/\lambda## follows that ##\Delta\omega \propto \Delta\lambda /\lambda^2 \propto \Delta\lambda (\omega/\lambda)##.
 
Orodruin said:
What you are saying is only true for the relationship between frequency and wavelength themselves - not their small variation.

From ##\omega \propto 1/\lambda## follows that ##\Delta\omega \propto \Delta\lambda /\lambda^2 \propto \Delta\lambda (\omega/\lambda)##.
Thank you. This tracks for me.
 
A somewhat cleaner derivation:

The product ##\omega\lambda## is constant so ##0=\Delta(\omega\lambda) \simeq \omega \Delta\lambda + \lambda\Delta\omega##. This directly leads to ##\Delta\lambda/\lambda \simeq - \Delta\omega/\omega##.
 
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