If we let h kTx, then kTxh and d (kTh) dx, so that
N 8 V
3
0
The definite integral is a standard one equal to 2.404. Inserting the numerical values of the other
quantities, with V1.00 cm^3 1.00 10 ^6 m^3 , we find that
N2.03 1010 photons
(b) The average energy of the photons is equal to the total energy per unit volume divided by
the number of photons per unit volume:
Since a 4 c(see the discussion of the Stefan-Boltzmann law later in this section) and
N(2.405) [8V(kThc)^3 ],
3.73 10 ^20 J0.233 eV
c^2 h^3 T
(2.405)(2k^3 )
aT^4
NV
0
u( ) d
n( )d
x^2 dx
ex 1
kT
hc
Statistical Mechanics 315
A thermograph measures the amount of infrared radiation each
small portion of a person's skin emits and presents this informa-
tion in pictorial form by different shades of gray or different colors
in a thermogram. The skin over a tumor is warmer than elsewhere
(perhaps because of increased blood flow or a higher metabolic
rate), and thus a thermogram is a valuable diagnostic aid for
detecting such maladies as breast and thyroid cancer. A small dif-
ference in skin temperature leads to a significant difference in
radiation rate.
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