Concept:
The self-inductance of a long solenoid depends on its number of turns, length, permeability of core material, and cross-sectional area.
For an air-core solenoid:
\[
L=\frac{\mu_0 N^2 A}{l}
\]
where:
- $L$ = self-inductance
- $\mu_0$ = permeability of free space
- $N$ = total number of turns
- $A$ = area of cross-section
- $l$ = length of solenoid
Step 1: Observe dependence on area
From the formula:
\[
L \propto A
\]
This means if cross-sectional area increases, self-inductance also increases in the same ratio.
Step 2: Reason physically
A larger cross-sectional area allows more magnetic flux to pass through each turn of the solenoid.
More magnetic flux linkage per unit current means greater self-inductance.
Step 3: If area changes
If area becomes $kA$, then:
\[
L'=\frac{\mu_0 N^2 (kA)}{l}=kL
\]
So inductance changes directly with area.
Examples:
- If area doubles $\Rightarrow L$ doubles
- If area becomes half $\Rightarrow L$ becomes half
Step 4: Final Answer
The self-inductance of a solenoid is directly proportional to its area of cross-section.
\[
\boxed{L \propto A}
\]
Quick Tip:
A wider solenoid stores more magnetic flux, so its inductance becomes larger.