Difference between revisions of "Aluminum Converter"
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The energy deposited per second: | The energy deposited per second: | ||
− | <math> (95.3125*10^6 \frac {MeV}{pulse})(300 \frac {pulses}{second} = 28.6*10^9 \frac {MeV}{second} </math> | + | <math> (95.3125*10^6 \frac {MeV}{pulse})(300 \frac {pulses}{second}) = 28.6*10^9 \frac {MeV}{second} </math> |
+ | ==Calculating the temperature increase== | ||
+ | |||
+ | The power deposited in 1/2 mil Al is: | ||
+ | |||
+ | <math> 28.6*10^9 \frac {MeV}{second} = (28.6*10^{15} \frac {eV}{second})(1.6*10^{-19} \frac {C}{eV} = 4.575*10^{-3} W </math> | ||
+ | |||
+ | Stefan-Boltzmann Law (Wien Approximation) says: | ||
+ | |||
+ | <math> P = (0.924)(Area)(\sigma)(T^4) </math> | ||
+ | |||
+ | Solving for Temperature and taking into account the two sides of the converter we get: | ||
+ | |||
+ | <math> T = (\frac {P}{(0.924)(2A)(\sigma)})^{\frac {1}{4}} </math> | ||
Revision as of 20:26, 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:
Assume a beam spot diameter on the converter surface of 5mm, or an area of .