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QJEEM24Ph18ea: JEE Main 2024 Physics - Class 12 JEEM24Ph18ea Solution: A monochromatic light of wavelength is incident on the single…

A monochromatic light of wavelength 6000 A˚6000 ~\mathring{A} is incident on the single slit of width 0.01 mm0.01 \mathrm{~mm} . If the diffraction pattern is formed at the focus of the convex lens of focal length 20 cm20 \mathrm{~cm} , the linear width of the central maximum is :

Multiple Choice Options

  • A 12 mm12 \mathrm{~mm}
  • B 24 mm24 \mathrm{~mm}
  • C 60 mm60 \mathrm{~mm}
  • D 120 mm120 \mathrm{~mm}

Step-by-Step Verified Solution

To find the linear width of the central maximum in a single-slit diffraction pattern, we can use the formula that relates the position of the first minima on either side of the central maximum. The angle, θ\theta , at which the first minimum occurs is given by:

asin⁡(θ)=mλa \sin(\theta) = m\lambda

Where:

  • aa is the width of the slit

  • λ\lambda is the wavelength of monochromatic light

  • mm is the order number of the minimum (for the first minimum, m=±1m = \pm 1 )

In our case, we want to find the position of the first minima to determine the width of the central maximum on the screen. So we will use m=1m = 1 and m=−1m = -1 which correspond to the first minima on either side of the central peak.

Given the width of the slit a=0.01a = 0.01 mm, which we need to convert to meters for consistency with the wavelength:

a=0.01×10−3ma = 0.01 \times 10^{-3} \text{m}

And the wavelength λ=6000A˚\lambda = 6000 \mathring{A} , also converting to meters:

λ=6000×10−10m\lambda = 6000 \times 10^{-10} \text{m}

We're using a convex lens of focal length f=20f = 20 cm to project the pattern onto a screen. We'll need to convert the focal length to meters as well:

f=20×10−2mf = 20 \times 10^{-2} \text{m}

We can calculate the angle θ\theta needed for the first minima using the approximation of small angles, where sin⁡(θ)≈θ\sin(\theta) \approx \theta :

aθ=mλa \theta = m\lambda

Now, solve for θ\theta for the first minimum (m = 1):

θ=λa\theta = \frac{\lambda}{a}

Plugging in the values:

θ=6000×10−100.01×10−3\theta = \frac{6000 \times 10^{-10}}{0.01 \times 10^{-3}}

θ=6000×10−1010−5\theta = \frac{6000 \times 10^{-10}}{10^{-5}}

θ=6000×10−5\theta = 6000 \times 10^{-5}

Now, linear width of the central maximum on the screen (from -m to m, or -1 to +1) will be twice the distance from the center to the first minimum, which can be found using the focal length of the lens ff and the angle θ\theta :

y=2fθy = 2f\theta

Plugging the focal length and calculated theta:

y=2×20×10−2×6000×10−5y = 2 \times 20 \times 10^{-2} \times 6000 \times 10^{-5}

y=40×10−2×6000×10−5y = 40 \times 10^{-2} \times 6000 \times 10^{-5}

y=240×10−3my = 240 \times 10^{-3} \text{m}

y=24×10−2my = 24 \times 10^{-2} \text{m}

y=24mmy = 24 \text{mm}

This means the linear width of the central maximum is 24 mm. Hence, the correct answer is Option B.

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