Average photon energy from a galaxy cluster

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Homework Help Overview

The discussion revolves around estimating the average photon energy from a galaxy cluster for an X-ray telescope, specifically the Chandra. The problem involves concepts of thermal bremsstrahlung and redshift, with a focus on the relationship between temperature and photon energy.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to calculate the average photon energy using integrals related to specific intensity and thermal bremsstrahlung, while also considering redshift effects. Some participants question the validity of starting integration at zero and the applicability of a single temperature for the emissions. Others suggest incorporating the sensitivity range of the Chandra telescope into the calculations.

Discussion Status

The discussion is active, with participants exploring different aspects of the problem. There is no explicit consensus on the approach, but guidance has been offered regarding the need for temperature values and the nature of the radiation involved.

Contextual Notes

Participants note the importance of the sensitivity range of the Chandra telescope and the distinction between thermal bremsstrahlung and black-body radiation. There are indications that certain assumptions about the radiation characteristics may need further clarification.

throneoo
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Homework Statement


I want to calculate/estimate the average photon energy from a galaxy cluster incident on the mirror of a X ray telescope (Chandra to be specific) . The cluster has redshift z and at constant uniform temperature T

Homework Equations


Specific Intensity of thermal bremsstrahlung : I∝Λ(ν)*T-1/2*exp(-hν/kT)
z=(νemittedobserved)/νobserved

The Attempt at a Solution


At high temperatures the X ray emission is dominated by thermal bremsstrahlung.
The average photon energy should be found via the integral ( ∫ I dν ) / ( ∫ [I/hν] dν ) from ν=0 to infinity, then that energy should be divided by (1+z) due to the redshift, but since the full expression is not given in the problem, it's not really a viable approach.

Therefore I'm left with the approximation approach. I think <E>=hv≈kT should be good enough since in the x-ray region, photons' momentum and energy is comparable to that of electrons, and that it seem to be the value at which I is equal to its average value (referring to the curve below).

The classical spectrum (valid for moderate temperature): https://upload.wikimedia.org/wikipe...ower2.svg/731px-Bremsstrahlung_power2.svg.png
 
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Galaxies radiate a lot more visible light than x-rays, and those two cannot be described by a single temperature. I don't think starting the integration at 0 will lead to a useful result.

You'll need a temperature value if you want to follow the approach of thermal emission. And probably the sensitivity range of Chandra, unless you really care about all the low-energetic photons.
 
Okay so I can effectively put the sensitivity range of chandra in my integration, then I~exp(-x) with the range. However exp(x)/x is still a nasty integral so I'll have to look up values of exponential integral.

And by thermal emission do you mean black-body emission?
 
If it is not black-body-like, you need to know more about the radiation.
 
I think that would be the braking radiation as given in OP
 

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