Difference between revisions of "Faraday Cup Temperature"
Jump to navigation
Jump to search
(6 intermediate revisions by the same user not shown) | |||
Line 5: | Line 5: | ||
Assume electron beam parameters at FC location are: | Assume electron beam parameters at FC location are: | ||
− | Frequency: f=300 Hz | + | Frequency: f = 300 Hz |
− | Peak current: I=3 Amps | + | Peak current: I = 3 Amps |
− | Pulse width: t= 50 ps | + | Pulse width: t = 50 ps |
− | Beam energy: E=45 MeV | + | Beam energy: E = 45 MeV |
The number of electrons per second at FC location are: | The number of electrons per second at FC location are: | ||
Line 17: | Line 17: | ||
<math> P = (0.28*10^{12}\ \frac{e}{sec}) (44\ MeV) (1.6*10^{-19} \frac{J}{eV}) = 1.9\ W</math> | <math> P = (0.28*10^{12}\ \frac{e}{sec}) (44\ MeV) (1.6*10^{-19} \frac{J}{eV}) = 1.9\ W</math> | ||
− | |||
==Temperature calculation== | ==Temperature calculation== | ||
Line 27: | Line 26: | ||
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. | ||
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\cdot 10^{-8} \frac {W}{m^2 K^4})} = 0. | + | <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})} = 0.1813\cdot10^{12}K^4</math> |
So | So | ||
− | <math> T = | + | <math> T = 652\ K </math> |
==Conclusion== | ==Conclusion== | ||
− | Because the melting point of Aluminum is | + | Because the melting point of Aluminum is 933.5 K we are safety. |
[http://wiki.iac.isu.edu/index.php/PhotoFission_with_Polarized_Photons_from_HRRL Go Back] | [http://wiki.iac.isu.edu/index.php/PhotoFission_with_Polarized_Photons_from_HRRL Go Back] |
Latest revision as of 05:49, 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
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 933.5 K we are safety.