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Question: Let \({{\text{k}}_1}\) be the maximum kinetic energy of photoelectrons emitted by a light of wavelen...

Let k1{{\text{k}}_1} be the maximum kinetic energy of photoelectrons emitted by a light of wavelength λ1{\lambda _1} and k2{{\text{k}}_2} responding to λ2{\lambda _2}, where λ1=2λ2{\lambda _1} = 2{\lambda _2}, then:
A) 2k1=k22{{\text{k}}_1} = {{\text{k}}_2}
B) k1 = 2k2{{\text{k}}_{\text{1}}}{\text{ = 2}}{{\text{k}}_{\text{2}}}
C) k1 < 2k2{{\text{k}}_{\text{1}}}{\text{ < 2}}{{\text{k}}_{\text{2}}}
D) k2>2k1{{\text{k}}_{\text{2}}} > 2{{\text{k}}_{\text{1}}}

Explanation

Solution

By the action of light, metal atoms emit electrons. If one is specific, then metal atoms emit electrons from the surface when light is incident on the surface. The phenomenon is termed the photoelectric effect, and the emitted electrons are called photoelectrons. The energy of these photoelectrons is significantly related to the property of the incident light.

Complete step by step solution:
Light Waves carry energy in the form of quanta or photons. When the light is incident on a photosensitive metal surface, metals emit electrons from its surface. The photons in the incident wave interact with the far most electron of an atom, resulting in emitted electrons from the metal surface. The metal surface emits electrons till the light is incident on the surface.
We use Einstein's Photoelectric Equation-
k=hνWk = h\nu - W…………….(1)(1)
Here, kk = maximum kinetic energy of the photoelectrons
hh is the Planck's constant
ν\nu is the frequency of the incident light
WW is the threshold energy, i.e., minimum work required to release photoelectrons
In (1)(1), we put ν=cλ\nu = \dfrac{c}{\lambda } and get-
k=hcλWk = \dfrac{{hc}}{\lambda } - W…………….(2)(2)
where λ\lambda is the wavelength of the incident light and
cc is the speed of light.
Now using equation (2)(2), we have-
k1=hcλ1W\Rightarrow {k_1} = \dfrac{{hc}}{{{\lambda _1}}} - W
k1=hc2λ2W\Rightarrow {k_1} = \dfrac{{hc}}{{2{\lambda _2}}} - W
hc2λ2=W+k1\Rightarrow \dfrac{{hc}}{{2{\lambda _2}}} = W + {k_1}…………(3)(3)
Also,
k2=hcλ2W\Rightarrow {k_2} = \dfrac{{hc}}{{{\lambda _2}}} - W
hcλ2=W+k2\Rightarrow \dfrac{{hc}}{{{\lambda _2}}} = W + {k_2}…………(4)(4)
We divide the equation (4)(4) by (2)(2) and then compare with the equation (3)(3)-
W+k1=W2+k22\Rightarrow W + {k_1} = \dfrac{W}{2} + \dfrac{{{k_2}}}{2}
2W+2k1=W+k2\Rightarrow 2W + 2{k_1} = W + {k_2}
k2=2k1+W\Rightarrow {k_2} = 2{k_1} + W
Hence, we have k2>2k1{k_2} > 2{k_1}

Therefore, the required answer is k2>2k1{k_2} > 2{k_1}, and option (D) is the correct answer.

Note: It is easier to emit electrons from atoms with lower threshold energy. The maximum kinetic energy of the photoelectrons is directly proportional to the frequency of the incident light. Again, the photoelectrons' maximum kinetic energy is inversely proportional to the wavelength of the incident light. Between a red light and blue light of the same intensity, the latter has more energy.