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Dual Nature of Radiation question

2013 · Shift 2 · Q47
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Dual Nature of Radiation question

2013 · Shift 2 · Q47

JEE AdvancedPhysicsDual Nature of RadiationMultiple correct+3 / −0.75
Using the expression 2dsin⁡θ=λ2d\sin \theta = \lambda2dsinθ=λ, one calculates the values of d by measuring the corresponding angles θ\thetaθ in the range 0 to 90o. The wavelength λ\lambdaλ is exactly known and the error in θ\thetaθ is constant for all values of θ\thetaθ. As θ\thetaθ increases from 0o
  1. A
    the absolute error in d remains constant
  2. B
    the absolute error in d increases
  3. C
    the fractional error in d remains constant
  4. D
    the fractional error in d decreases
View written solutionFree

Correct answer: D

  1. We are given Bragg’s law:

2dsin⁡θ=λ2d\sin\theta = \lambda2dsinθ=λ

Since λ\lambdaλ is exactly known,

d=λ2sin⁡θd = \frac{\lambda}{2\sin\theta}d=2sinθλ​

We need to see how the error in ddd depends on θ\thetaθ, given that the error in θ\thetaθ is constant.


  1. Use error propagation.

For small errors,

Δd≈∣dddθ∣Δθ\Delta d \approx \left|\frac{dd}{d\theta}\right| \Delta\thetaΔd≈​dθdd​​Δθ

Now,

d=λ2sin⁡θ=λ2csc⁡θd = \frac{\lambda}{2\sin\theta} = \frac{\lambda}{2}\csc\thetad=2sinθλ​=2λ​cscθ

Differentiate with respect to θ\thetaθ:

dddθ=λ2(−csc⁡θcot⁡θ)\frac{dd}{d\theta} = \frac{\lambda}{2}(-\csc\theta\cot\theta)dθdd​=2λ​(−cscθcotθ)

So,

∣dddθ∣=λ2csc⁡θcot⁡θ\left|\frac{dd}{d\theta}\right| = \frac{\lambda}{2}\csc\theta\cot\theta​dθdd​​=2λ​cscθcotθ

Hence the absolute error is

Δd≈λ2csc⁡θcot⁡θ Δθ\Delta d \approx \frac{\lambda}{2}\csc\theta\cot\theta\,\Delta\thetaΔd≈2λ​cscθcotθΔθ

or equivalently,

Δd∝csc⁡θcot⁡θ=cos⁡θsin⁡2θ\Delta d \propto \csc\theta\cot\theta = \frac{\cos\theta}{\sin^2\theta}Δd∝cscθcotθ=sin2θcosθ​

As θ\thetaθ increases from 0∘0^\circ0∘ to 90∘90^\circ90∘, sin⁡θ\sin\thetasinθ increases and cos⁡θ\cos\thetacosθ decreases, so

cos⁡θsin⁡2θ\frac{\cos\theta}{\sin^2\theta}sin2θcosθ​

decreases.

Therefore, the absolute error in ddd decreases with increasing θ\thetaθ.

So:

  • A is false
  • B is false

  1. Now find the fractional error.

Δdd≈∣1ddddθ∣Δθ\frac{\Delta d}{d} \approx \left|\frac{1}{d}\frac{dd}{d\theta}\right|\Delta\thetadΔd​≈​d1​dθdd​​Δθ

Using d=λ2csc⁡θd = \frac{\lambda}{2}\csc\thetad=2λ​cscθ,

Δdd=λ2csc⁡θcot⁡θ Δθλ2csc⁡θ\frac{\Delta d}{d} = \frac{\frac{\lambda}{2}\csc\theta\cot\theta\,\Delta\theta}{\frac{\lambda}{2}\csc\theta}dΔd​=2λ​cscθ2λ​cscθcotθΔθ​

This gives

Δdd=cot⁡θ Δθ\frac{\Delta d}{d} = \cot\theta\,\Delta\thetadΔd​=cotθΔθ

Since Δθ\Delta\thetaΔθ is constant,

Δdd∝cot⁡θ\frac{\Delta d}{d} \propto \cot\thetadΔd​∝cotθ

As θ\thetaθ increases from 0∘0^\circ0∘ to 90∘90^\circ90∘, cot⁡θ\cot\thetacotθ decreases.

Therefore, the fractional error in ddd decreases.

So:

  • C is false
  • D is true

  1. Final option check:
  • A: False
  • B: False
  • C: False
  • D: True

Thus the correct answer is:

D\boxed{D}D​

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