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Physics
The wavelength of a photon needed to remove a proton from a nucleus which is bound to the nucleus with 1 MeV energy is nearly
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Q. The wavelength of a photon needed to remove a proton from a nucleus which is bound to the nucleus with $1\, MeV$ energy is nearly
Dual Nature of Radiation and Matter
A
$1.2\,nm$
13%
B
$1.2 \times 10^{-3}\,nm$
54%
C
$1.2 \times 10^{-6}\,nm$
28%
D
$1.2 \times 10^1\,nm$
5%
Solution:
Here, $E = 1 \,MeV = 10^{6}eV$,
$ h = 6.63 \times10^{-34} \,J\, s$,
$ c= 3\times10^{8} \,m \,s^{-1} $
$ \therefore hc = \frac{6.63 \times 10^{-34} \times 3\times 10^{8}}{1.6 \times 10^{-9}} \approx 1240 \,eV \,nm$
As $E =\frac{hc}{\lambda}$
or $\lambda = \frac{hc}{E} =\frac{ 1240\, eV \,nm }{10^{6} eV}$
$ = 1.24 \times 10^{-3}\, nm$