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 have
Where 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 .