Difference between revisions of "Aluminum Converter"
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<math> T^4 = \frac {P}{(0.924)(2A)(\sigma)} </math> | <math> T^4 = \frac {P}{(0.924)(2A)(\sigma)} </math> | ||
− | where <math> \sigma </math> is the Stefan-Boltzmann constant, <math> \sigma = 5.67*10^{-8} \frac {W}{m^2 K^4}. Assume a beam spot diameter on the converter surface of 5mm, or an area of <math> A = 19.62 mm^2 = 19.62*10^{-6} m^2 </math>. | + | where <math> \sigma </math> is the Stefan-Boltzmann constant, <math> \sigma = 5.67*10^{-8} \frac {W}{m^2 K^4} </math>. Assume a beam spot diameter on the converter surface of 5mm, or an area of <math> A = 19.62 mm^2 = 19.62*10^{-6} m^2 </math>. |
Revision as of 20:33, 7 June 2010
Calculating the temperature of a 1/2 mil Aluminum converter with energy deposited from a 44 MeV electron beam.
Calculating number of particles per second
We have electron beam of:
Frequency:
Peak current:
Pulse width:
By
, we haveWhere
is the number of electrons that hit the target per second, is electron charge and , and are given above.
So, we have around
electrons per second or electrons per pulse.Calculating the stopping power due to collision of one 44 MeV electron in Aluminum
From NIST ([1] see link here) the stopping power for one electron with energy of 44 MeV in Aluminum is .
The effective length of 1/2 mil Al:
The total stopping power due to collisions on Al per incident electron:
The energy deposited per pulse:
The energy deposited per second:
Calculating the temperature increase
The power deposited in 1/2 mil Al is:
Stefan-Boltzmann Law (Wien Approximation) says
Solving for Temperature and taking into account the two sides of the converter we get:
where
is the Stefan-Boltzmann constant, . Assume a beam spot diameter on the converter surface of 5mm, or an area of .