According to the Richardson-Dushman equation, the number of thermions emitted per second by a surface at temperature
T is given by:
n(T)∝T2e−kBTWThe ratio of the number of thermions emitted at temperature
T to that at
1000 K is:
n(1000)n(T)=(1000T)2e−kBW(T1−10001)Given the work function
W=4.52 eV and the Boltzmann constant
kB≈8.62×10−5 eV/K, we have:
kBW=8.62×10−54.52≈52436 KFor
T=300 K:
n(1000)n(300)=(1000300)2e−52436(3001−10001)n(1000)n(300)=0.09×e−122.35≈0.09×7.30×10−54=6.57×10−55For
T=2000 K:
n(1000)n(2000)=(10002000)2e−52436(20001−10001)n(1000)n(2000)=4×e26.218≈4×2.43×1011=9.73×1011For
T=3000 K:
n(1000)n(3000)=(10003000)2e−52436(30001−10001)n(1000)n(3000)=9×e34.957≈9×1.52×1015=1.37×1016Answer:
6.57×10−55,
9.73×1011,
1.37×1016