Faraday Cup Temperature: Difference between revisions
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Here, | Here, | ||
A is the radiated area of the rode | A is the radiated area of the rode | ||
<math> \sigma = 5.67\cdot 10^{-8} \frac {W}{m^2 K^4} </math> is the Stefan-Boltzmann constant. | <math> \sigma = 5.67\cdot 10^{-8} \frac {W}{m^2 K^4} </math> is the Stefan-Boltzmann constant. | ||
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<math> T = 424\ K </math> | <math> T = 424\ K </math> | ||
==Conclusion== | ==Conclusion== | ||
Revision as of 05:32, 14 October 2010
Calculating the temperature of a Faraday Cup Rod
Number of particles per second and corresponding beam power
Assume electron beam parameters at FC location are:
Frequency: f=300 Hz Peak current: I=3 Amps Pulse width: t= 50 ps Beam energy: E=45 MeV
The number of electrons per second at FC location are:
[math]\displaystyle{ N = \frac {Q} {e} = \frac {f I ∆t} {e} = \frac {(300\ Hz)(3\ A) (50\ ps)} {1.6*10^{-19}\ C} = 0.28*10^{12} }[/math]
The corresponding beam power for 45 MeV electron beam is:
[math]\displaystyle{ P = (0.28*10^{12}\ \frac{e}{sec}) (44\ MeV) (1.6*10^{-19} \frac{J}{eV}) = 1.9\ W }[/math]
Temperature calculation
Now apply the Stefan-Boltzmann Law for one Faraday cup rod
[math]\displaystyle{ P = (0.924)\ (A)\ (\sigma)\ (T^4) }[/math]
Here,
A is the radiated area of the rode
[math]\displaystyle{ \sigma = 5.67\cdot 10^{-8} \frac {W}{m^2 K^4} }[/math] is the Stefan-Boltzmann constant.
Assume the all beam power goes to one FC rod and area of radiation is 2 cm^2 (two back sides) we can calculate the corresponding temperature:
[math]\displaystyle{ T^4 = \frac {P}{0.924\ A\ \sigma} = \frac {1.9\ W}{(0.924)(2\cdot 10^{-4}\ m^2)(5.67\cdot 10^{-8} \frac {W}{m^2 K^4})} = 0.18\cdot10^{12}K^4 }[/math]
So
[math]\displaystyle{ T = 424\ K }[/math]
Conclusion
Because the melting point of Aluminum is [math]\displaystyle{ 933.5 K }[/math] we are safety.