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Dual Nature of Radiation question

2023 · 25 Jan · Shift 1 · Q56
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  5. /2023 · 25 Jan · Shift 1 · Q56

Dual Nature of Radiation question

2023 · 25 Jan · Shift 1 · Q56

JEE MainPhysicsDual Nature of RadiationMCQ+4 / −1
Electron beam used in an electron microscope, when accelerated by a voltage of 20 kV, has a de-Broglie wavelength of λ0\lambda_0λ0​. IF the voltage is increased to 40 kV, then the de-Broglie wavelength associated with the electron beam would be :
  1. A
    3 λ0\lambda_0λ0​
  2. B
    9 λ0\lambda_0λ0​
  3. C
    λ02\frac{\lambda_0}{\sqrt2}2​λ0​​
  4. D
    λ02\frac{\lambda_0}{2}2λ0​​
View written solutionFree

Correct answer: C

  1. For an electron accelerated through a potential difference VVV, its de-Broglie wavelength is
λ=hp\lambda = \frac{h}{p}λ=ph​

For non-relativistic electrons,

p22m=eV\frac{p^2}{2m} = eV2mp2​=eV

So,

p=2meVp = \sqrt{2meV}p=2meV​

Hence,

λ=h2meV\lambda = \frac{h}{\sqrt{2meV}}λ=2meV​h​

This shows that

λ∝1V\lambda \propto \frac{1}{\sqrt{V}}λ∝V​1​
  1. Initially, at voltage V1=20 kVV_1 = 20\,\text{kV}V1​=20kV, the wavelength is λ0\lambda_0λ0​.

When the voltage is increased to

V2=40 kVV_2 = 40\,\text{kV}V2​=40kV

we use

λ2λ1=V1V2\frac{\lambda_2}{\lambda_1} = \sqrt{\frac{V_1}{V_2}}λ1​λ2​​=V2​V1​​​

Thus,

λ2λ0=2040=12=12\frac{\lambda_2}{\lambda_0} = \sqrt{\frac{20}{40}} = \sqrt{\frac{1}{2}} = \frac{1}{\sqrt{2}}λ0​λ2​​=4020​​=21​​=2​1​

Therefore,

λ2=λ02\lambda_2 = \frac{\lambda_0}{\sqrt{2}}λ2​=2​λ0​​
  1. Checking options:
  • A: 3λ03\lambda_03λ0​ ❌
  • B: 9λ09\lambda_09λ0​ ❌
  • C: λ02\dfrac{\lambda_0}{\sqrt2}2​λ0​​ ✅
  • D: λ02\dfrac{\lambda_0}{2}2λ0​​ ❌

So the correct option is C.

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