Uniform field \( \vec E = E\hat i \). Compare potentials at A(0,0), B(1 cm,0), C(0,1 cm).
Potential drops along field lines, unchanged along equipotentials.
\(V_A > V_B\) and \(V_C = V_A\).
👍/👎 Does \(V_C = V_A\)?
Source: CBSE Sample Paper 2024-25
CBSE SQP Q2: Equal potential ⇒ compare surface fields.
Wire joins two distant metal spheres; charges flow until both sit at the same potential \(V\).
\(kQ_1/r_1 = kQ_2/r_2\) ⇒ \(Q_1/Q_2 = r_1/r_2\).
With \(E = kQ/r^{2}\), we get \(E_1/E_2 = r_2/r_1\). The smaller sphere feels the stronger field (Option B).
Equal potential does not imply equal field—the field scales inversely with radius here.
Inside, \(B\propto r\); cross the surface and \(B\propto 1/r\). Ampere’s law applies in both zones.
Find \( |B| \) at \(1.5a\) ( \(a/2\) above surface ) and at \(0.5a\) (inside). Give the ratio.
\(B_{\text{out}} = \mu_{0}I/3\pi a\), \(B_{\text{in}} = \mu_{0}I/4\pi a\) ⇒ ratio \(4:3\).
Vote: 1 : 1, 4 : 3, or 3 : 4 — which is correct?
Source: CBSE Sample Question Paper 2024-25 (Q3)
Rainbow diffraction on a CD
Your voice curving round a corner and the rainbow sheen on a CD are both produced by diffraction.
The effect appears whenever the size of an opening or obstacle matches the wavelength.
Recall these must-know formulas & patterns for Q1–Q4
Potential drops linearly: \( \Delta V = -E\,\Delta x \).
At equilibrium \( V_1 = V_2 \); surface field varies as \( E \propto 1/r \).
Magnetic field: inside \( B \propto r \); outside \( B \propto 1/r \).
Noticeable when aperture ≈ wavelength—true for all waves.