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Dual Nature of Radiation question

2024 · 31 Jan · Shift 1 · Q69
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  5. /2024 · 31 Jan · Shift 1 · Q69

Dual Nature of Radiation question

2024 · 31 Jan · Shift 1 · Q69

JEE MainPhysicsDual Nature of RadiationMCQ+4 / −1
When a metal surface is illuminated by light of wavelength λ\lambdaλ, the stopping potential is 8 V8 \mathrm{~V}8 V. When the same surface is illuminated by light of wavelength 3λ3 \lambda3λ, stopping potential is 2 V2 \mathrm{~V}2 V. The threshold wavelength for this surface is:
  1. A
    3 λ\lambdaλ
  2. B
    9 λ\lambdaλ
  3. C
    5 λ\lambdaλ
  4. D
    4.5 λ\lambdaλ
View written solutionFree

Correct answer: B

  1. Use Einstein’s photoelectric equation

For incident light of wavelength λ\lambdaλ,

hcλ=ϕ+eVs\frac{hc}{\lambda} = \phi + eV_sλhc​=ϕ+eVs​

where ϕ\phiϕ is the work function and VsV_sVs​ is the stopping potential.

It is often convenient to write

eVs=hc(1λ−1λ0)eV_s = hc\left(\frac{1}{\lambda}-\frac{1}{\lambda_0}\right)eVs​=hc(λ1​−λ0​1​)

where λ0\lambda_0λ0​ is the threshold wavelength.


  1. Write equations for the two cases

Case 1:

When wavelength is λ\lambdaλ, stopping potential is 8 V8\,\text{V}8V:

e(8)=hc(1λ−1λ0)e(8)=hc\left(\frac{1}{\lambda}-\frac{1}{\lambda_0}\right)e(8)=hc(λ1​−λ0​1​)

Case 2:

When wavelength is 3λ3\lambda3λ, stopping potential is 2 V2\,\text{V}2V:

e(2)=hc(13λ−1λ0)e(2)=hc\left(\frac{1}{3\lambda}-\frac{1}{\lambda_0}\right)e(2)=hc(3λ1​−λ0​1​)
  1. Eliminate constants by dividing/subtracting

Let

K=hceK=\frac{hc}{e}K=ehc​

Then the equations become

8=K(1λ−1λ0)8 = K\left(\frac{1}{\lambda}-\frac{1}{\lambda_0}\right)8=K(λ1​−λ0​1​) 2=K(13λ−1λ0)2 = K\left(\frac{1}{3\lambda}-\frac{1}{\lambda_0}\right)2=K(3λ1​−λ0​1​)

Subtract the second equation from the first:

8−2=K(1λ−13λ)8-2 = K\left(\frac{1}{\lambda}-\frac{1}{3\lambda}\right)8−2=K(λ1​−3λ1​) 6=K(23λ)6 = K\left(\frac{2}{3\lambda}\right)6=K(3λ2​) K=9λK = 9\lambdaK=9λ

Now substitute into the second equation:

2=9λ(13λ−1λ0)2 = 9\lambda\left(\frac{1}{3\lambda}-\frac{1}{\lambda_0}\right)2=9λ(3λ1​−λ0​1​) 2=3−9λλ02 = 3 - \frac{9\lambda}{\lambda_0}2=3−λ0​9λ​ 9λλ0=1\frac{9\lambda}{\lambda_0}=1λ0​9λ​=1 λ0=9λ\lambda_0 = 9\lambdaλ0​=9λ
  1. Check with first equation
8=9λ(1λ−19λ)=9(1−19)=9⋅89=88 = 9\lambda\left(\frac{1}{\lambda}-\frac{1}{9\lambda}\right) =9\left(1-\frac{1}{9}\right)=9\cdot\frac{8}{9}=88=9λ(λ1​−9λ1​)=9(1−91​)=9⋅98​=8

Correct.


  1. Final answer

Threshold wavelength is

9λ\boxed{9\lambda}9λ​

So the correct option is B.

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