With the information of the beam, we can find the number of protons if we know that the charge is equal to the charge of the proton times the number of protons:
I=ΔtΔQ=ΔtNpqproton⟹Np=qprotonIΔt
After that analysis we also have to calculate the energy of the beam, we use the equation for the kinetic energy of a single traveling proton and we find the total energy of the beam as the kinetic energy times the number of protons:
Ekinetic=21mprotonv2ET=NpEkinetic=2qproton(IΔt)mprotonv2
Then, since only a third of the total energy is converted into heat we can relate that to the heat capacity and mass of the target, after substitution we find the temperature variation on the target as:
Q=31ET=6qproton(IΔt)mprotonv2=MtargetCtargetΔT⟹ΔT=6qprotonMtargetCtarget(IΔt)mprotonv2
ΔT=6(1.609×10−19C)(1g)(0.334cal/gK)(4.184J/cal)(4.8×10−6A)(1s)(1.67×10−27kg))(2×107m/s)2
After substitution this gives the temperature variation in Kelvin:
ΔT=6(1.609)(1)(0.334)(4.184)(4.8)(1)(1.67))(2)2KΔT=2.3767K
In conclusion, the temperature variation of the target in a time interval ∆t = 1 s is ΔT=2.3767K.
Reference:
- Young, H. D., & Freedman, R. A. (2015). University Physics with Modern Physics and Mastering Physics (p. 1632). Academic Imports Sweden AB.
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