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Question: Light of wavelength 2200 \(\overset{\circ }{\mathop{A}}\,\) (angstrom) falls on a photosensitive pla...

Light of wavelength 2200 A\overset{\circ }{\mathop{A}}\, (angstrom) falls on a photosensitive plate with work function 4.1 eV. Find (a) energy of a photon in eV (electron volt). (b) maximum kinetic energy of photoelectron and (c) stopping potential.

Explanation

Solution

Hint: Energy of a photon is given as E=hνE=h\nu . Use the relation between speed of light, its frequency and its wavelength to find the energy of a photon in eV. Maximum kinetic energy of the photoelectron is given as Kmax=hvϕ{{K}_{\max }}=hv-\phi .

Formula used:
E=hνE=h\nu
Kmax=hvϕ{{K}_{\max }}=hv-\phi
ν=cλ\nu =\dfrac{c}{\lambda }
1eV=1.6×1019J1eV=1.6\times {{10}^{-19}}J
W = qV

Complete step-by-step answer:
It is considered that light is made up of small energy packets called photons. You can think of a photon as a particle with no mass. However, a photon has momentum. The energy of a photon is given as E=hνE=h\nu , where h is Planck’s constant and ν\nu is frequency of light.
When a beam of light falls on a metal, the photons collide with the electrons at the surface of the metal and transfer their energy to the electrons. If the electrons absorb more than a certain amount of energy (called work function), they get free from the electrostatic force and come out of the metal with some kinetic energy. This electron is called a photoelectron.
The maximum kinetic energy of an electron is given as Kmax=hvϕ{{K}_{\max }}=hv-\phi ,
where hvhv is the energy of the photon and ϕ\phi is the amount of energy needed to break the bond between the electron and the nucleus.
Let us now calculate the things that are asked in the question.

(a) Energy of a photon is E=hνE=h\nu .
Let us assume that this experiment is taking place in vacuum then,
ν=cλ\nu =\dfrac{c}{\lambda }, where c is the speed of light in vacuum and λ\lambda is the wavelength of light.
Therefore,
E=hcλE=h\dfrac{c}{\lambda }.
Here, h=6.62×1034Jsh=6.62\times {{10}^{-34}}Js, c=3×108ms1c=3\times {{10}^{8}}m{{s}^{-1}} and λ=2200A=2200×108m\lambda =2200\overset{\circ }{\mathop{A}}\,=2200\times {{10}^{-8}}m
Therefore,
E=6.62×1034Js.3×108ms12200×108m=0.9×1018JE=6.62\times {{10}^{-34}}Js.\dfrac{3\times {{10}^{8}}m{{s}^{-1}}}{2200\times {{10}^{-8}}m}=0.9\times {{10}^{-18}}J ……(i).s
1eV=1.6×1019J1J=11.6×1019eV1eV=1.6\times {{10}^{-19}}J\Rightarrow 1J=\dfrac{1}{1.6\times {{10}^{-19}}}eV
Substitute the value of 1J in equation (i).
E=0.9×1018.11.6×1019eV=5.6eVE=0.9\times {{10}^{-18}}.\dfrac{1}{1.6\times {{10}^{-19}}}eV=5.6eV
Hence, the energy of the photons is 5.6eV.

(b) Maximum kinetic energy of the photoelectron is
Kmax=hvϕ{{K}_{\max }}=hv-\phi
We just found the value of hv, which is equal to 5.6eV and it is given that ϕ=4.1eV\phi =4.1eV.
Therefore,
Kmax=5.64.1=1.5eV{{K}_{\max }}=5.6-4.1=1.5eV.
Hence, the maximum kinetic energy of the electron is 1.5eV.

(c) Stopping potential is a potential difference that is created to stop the motion electron.
Here the electron has a kinetic energy of 1.5eV. Therefore, a negative work must be done on the electron to bring it to rest.
Let that potential difference be P. Since, W=qV, if the electron travels through a potential difference of P, a work will be done on it equal to eP.
Therefore, Kmax=eP=1.5eV{{K}_{\max }}=eP=1.5eV
P=1.5V\Rightarrow P=1.5V.
Hence, the stopping potential in this case is 1.5V.

Note: One photon can eject only one electron at a time. And the electron will eject out of the metal only if the energy of that photon is more than the work function of the metal.
Not every photoelectron possesses a kinetic energy equal to Kmax{{K}_{\max }}, because there are a lot of factors that influence the motion of the electron, such as repulsion due to other electrons, electron collide with each other dissipating some amount of energy.