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Question: When a metal surface is illuminated by light of wavelengths \(400nm\) and \(250nm\), the maximum vel...

When a metal surface is illuminated by light of wavelengths 400nm400nm and 250nm250nm, the maximum velocities of the photoelectrons ejected are VV and 2V2V respectively. The work function of the metal is
A. 2hc×106J2hc \times {10^6}J
B. 1.5hc×106J1.5hc \times {10^6}J
C. hc×106Jhc \times {10^6}J
D. 0.5hc×106J0.5hc \times {10^6}J

Explanation

Solution

The equation for maximum kinetic energy of the photoelectrons ejected as a result of photoelectric emission is given as KE=EWKE = E - W, KEKE is the kinetic energy of the photoelectrons (KE=12mv2)\left( {KE = \dfrac{1}{2}m{v^2}} \right), WW is the work function of the metals surface and EE is energy of the incident light(E=hcλ)\left( {E = \dfrac{{hc}}{\lambda }} \right).Upon substituting the values given in the question and solving the question we get the value of work function.

Complete step by step answer:
We know that the energy of light can be written as E=hcλE = \dfrac{{hc}}{\lambda }.
where hh is Planck's constant, cc is the speed of light and λ\lambda is the wavelength of light.
The equation for maximum kinetic energy of photoelectrons emitted as a result of photoelectric emission is KE=EWKE = E - W,
We know that the kinetic energy is written as (KE=12mv2)\left( {KE = \dfrac{1}{2}m{v^2}} \right),
where mm is the mass and vv is the velocity of the photoelectron.
Therefore the equation becomes,
12mv2=hcλW\dfrac{1}{2}m{v^2} = \dfrac{{hc}}{\lambda } - W -----------(1)
Given when the wavelength of light is 400nm then the maximum velocity of photoelectron is V. Substituting these values in the equation 1 we get,
12mV2=hc400W\dfrac{1}{2}m{V^2} = \dfrac{{hc}}{{400}} - W -------------(2)

When the wavelength of light is 250nm then the maximum velocity of the photoelectron is 2V. Substituting these values in the equation 1 we get,
12m4V2=hc250W\dfrac{1}{2}m4{V^2} = \dfrac{{hc}}{{250}} - W -------------(3)
Multiplying to 4 equation 2
12m4V2=hc1004W\dfrac{1}{2}m4{V^2} = \dfrac{{hc}}{{100}} - 4W --------------(4)
Subtracting equation 4 from 3 we get
0=3hc(500)nm+3W 3W=3hc(500)nm W=hc500×109(1nm=109m) W=2hc×106J 0 = - \dfrac{{3hc}}{{(500)nm}} + 3W \\\ \Rightarrow 3W = \dfrac{{3hc}}{{(500)nm}} \\\ \Rightarrow W = \dfrac{{hc}}{{500}} \times {10^9}\left( {1nm = {{10}^{ - 9}}m} \right) \\\ \therefore W = 2hc \times {10^6}J \\\

Hence, the work function of the metal is 2hc×106J2hc \times {10^6}J.

Note: We know that metal has free electrons (negatively charged particles) in its surface. But free electrons cannot escape from the metal surface unless there is a push or pull. If electrons attempt to escape from the surface of the metal, it will acquire a positive charge hence it will attract back the electrons to the surface. So as mentioned earlier it requires sufficient energy to overcome the attractive pull. A certain amount of energy is required for an electron to pull it out from the surface of the metal. That minimum energy required is known as the work function of the metal.