Difference between revisions of "Faraday Cup Temperature"
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A is the radiated area of the rode.radiatedanradiated | A is the radiated area of the rode.radiatedanradiated | ||
− | <math> \sigma = 5.67 | + | <math> \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: | 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> T^4 = \frac {P}{0.924\ A\ \sigma} = \frac {1.9\ W}{(0.924)(2\cdot 10^{-4}\ m^2)(5.67\ 10^{-8} \frac {W}{m^2 K^4})} = 0.18\ K^4</math> | + | <math> 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\ K^4</math> |
So | So |
Revision as of 05:29, 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:
The corresponding beam power for 45 MeV electron beam is:
Temperature calculation
Now apply the Stefan-Boltzmann Law for one Faraday cup rod
Here,
A is the radiated area of the rode.radiatedanradiated
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:
So
Conclusion
Because the melting point of Aluminum is
we are safety.