Concept:
For Fraunhofer diffraction due to a single slit of width $d$:
\[
W=\frac{2\lambda D}{d}
\]
where:
- $W$ = linear width of central maximum
- $\lambda$ = wavelength of light
- $D$ = distance of screen from slit
- $d$ = slit width
Hence, width of central maximum is inversely proportional to slit width:
\[
W \propto \frac{1}{d}
\]
Also, the amplitude at the center is proportional to slit width, therefore intensity is:
\[
I \propto d^2
\]
Step 1: Given change in slit width
Original slit width:
\[
d
\]
New slit width after doubling:
\[
d' = 2d
\]
Step 2: Find new angular / linear width of central maximum
Since:
\[
W \propto \frac{1}{d}
\]
Therefore:
\[
W'=\frac{W}{2}
\]
So, the width of the central maximum becomes half of its original value.
Step 3: Find new intensity
Since:
\[
I \propto d^2
\]
Then:
\[
I' \propto (2d)^2 = 4d^2
\]
Thus:
\[
I' = 4I
\]
So, the intensity becomes four times the original intensity.
Step 4: Final Result
When the slit width is doubled:
- Width of central maximum becomes half.
- Intensity of central maximum becomes four times.
\[
\boxed{W'=\frac{W}{2}, \qquad I'=4I}
\]
Quick Tip:
In diffraction, increasing slit width makes the pattern narrower but brighter.