Animated Solution for Physics - Optics: Visible light of wavelength 6000×10−8 cm falls normally on a single slit and produces a diffraction pattern. It is found that the second diffraction minimum is at 60∘ from the central maximum. If the first minimum is produced at θ1, then θ1 is close to
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Visualized Solution
Single Slit Setup
Single Slit Diffraction Setup
Condition for Minima
Condition for nth minimum:
Dsinθn=nλ
⇒sinθn=Dnλ
Second Minimum Data
For the 2nd minimum (n=2):
θ2=60∘
sin60∘=D2λ
Calculating Dλ
Dλ=2sin60∘
Dλ=23/2≈20.866
Dλ≈0.433
First Minimum Setup
For the 1st minimum (n=1):
sinθ1=D1⋅λ=Dλ
Final Calculation
sinθ1≈0.433
Given sin25∘=0.422
⇒θ1≈25∘
The Way Forward
Extra data in questions can be a trap!
Always simplify equations before substituting values.
Food for thought: What happens to θ1 if D is halved?
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The Sigma Insight: Diffraction due to Single Slit
Solution Diagram
Unraveling the Single Slit Diffraction Pattern
Imagine a beam of light passing through a narrow slit. Instead of just creating a sharp shadow, the light spreads out, creating a beautiful pattern of alternating bright and dark bands on a screen. This phenomenon is known as diffraction. In this problem, we are dealing with a classic single-slit diffraction setup, and our goal is to find the angular position of the first dark band (minimum) given the position of the second one.
The Master Equation
The key to unlocking any single-slit diffraction problem is the condition for the formation of minima (dark fringes). The angular position θn of the nth minimum is governed by the equation:
Dsinθn=nλ
Here, D is the width of the slit, λ is the wavelength of the incident light, and n is an integer (1,2,3,…) representing the order of the minimum.
Decoding the Second Minimum
The problem provides us with a crucial piece of information: the second diffraction minimum (n=2) occurs at an angle of 60∘. Let's plug these values into our master equation:
Dsin60∘=2λ
From this, we can isolate the ratio of the wavelength to the slit width, Dλ. This ratio is a constant for the given setup and will be the stepping stone to our final answer.
Dλ=2sin60∘
We know that sin60∘=23≈0.866. Substituting this value, we get:
Dλ≈20.866=0.433
Finding the First Minimum
Now, we need to find the angular position of the first minimum, which we'll call θ1. For the first minimum, n=1. Applying our master equation again:
Dsinθ1=1⋅λ
sinθ1=Dλ
We already calculated the value of Dλ in the previous step! Let's substitute it here:
sinθ1≈0.433
To find θ1, we need to determine which angle has a sine value close to 0.433. Looking at the standard trigonometric values, we know sin30∘=0.5. Since 0.433 is less than 0.5, the angle must be less than 30∘.
If we look at the given options, 25∘ is a very strong candidate. In fact, sin25∘≈0.422, which is remarkably close to our calculated value of 0.433. Therefore, we can confidently conclude that:
θ1≈25∘
The Trap of Extra Data
Did you notice something interesting? The problem explicitly gave us the wavelength of the light (λ=6000×10−8 cm). However, we arrived at the correct answer without ever plugging this number into our calculations!
This is a classic trap in competitive exams like JEE. Examiners often provide redundant information to test your conceptual clarity and see if you can identify the most efficient path to the solution. By working with ratios instead of absolute values, we saved time and avoided messy calculations. Always simplify your equations algebraically before reaching for the numbers!