Match chapter-wise question load with your proficiency to target revision smartly.
| Chapter (Syllabus) | Questions in Paper | Your Strength |
|---|---|---|
| Electric Charges & Fields | 3 | Low |
| Moving Charges & Magnetism | 4 | Low |
| Alternating Current | 2 | Low |
| Wave Optics | 3 | Low |
| Nuclei | 2 | Low |
| Electrostatic Potential & Capacitance | 2 | Med |
| Magnetism & Matter | 0 | Med |
| Electromagnetic Waves | 1 | Med |
| Dual Nature of Radiation & Matter | 2 | Med |
| Semiconductor Electronics | 3 | Med |
| Current Electricity | 4 | High |
| Electromagnetic Induction | 1 | High |
| Ray Optics & Optical Instruments | 3 | High |
| Atoms | 1 | High |
Source: CBSE Grade 12 Self-assessment, 2024 Paper
Electric Charges & Fields – Gauss’s Law Application
Using Gauss’s law, derive the electric field \(E(r)\) at distance \(r\) from an infinitely long straight wire carrying linear charge density \( \lambda \).
Imagine a coaxial cylindrical Gaussian surface.
Think of a Gaussian surface that shares the wire’s cylindrical symmetry.
Enclose length \(L\) of wire inside a coaxial cylinder of radius \(r\); ignore the flat caps.
Apply \( \Phi = E(2\pi r L) = \lambda L / \varepsilon_0 \). Solve to get \( E = \dfrac{\lambda}{2\pi \varepsilon_0 r} \). Do not count end-caps.
Identify symmetry, choose surface, compute flux, then isolate \(E\).
Recall the Gauss’s-law derivation for an infinite plane to spot parallels.
Sketch the wire and a dashed cylindrical surface to see where flux exits.
Check if \(E \propto 1/r\); doubling \(r\) should halve your answer.
Struggle is normal! Try to solve on your own before checking the hints.
Grade 12 Physics – Moving Charges & Magnetism
A \(+10\;\text{mC}\), \(10\;\text{g}\) sphere inside a vertical insulating tube stays at rest while the tube slides horizontally east → west through a uniform \(2\;\text{T}\) magnetic field. Find (i) the minimum tube speed and (ii) the field direction that keeps the sphere suspended.
No diagram required
Identify all forces and set their vector sum to zero.
Use \(qvB\) upward to cancel \(mg\) downward; thus \(qvB = mg\).
Solve \(v = \frac{mg}{qB} = \frac{0.01 \times 9.8}{0.01 \times 2} = 4.9\;\text{m s}^{-1}\). For a westward \( \mathbf{v} \) and positive \(q\), \( \mathbf{B} \) must point south so that \( \mathbf{v}\times\mathbf{B} \) is upward.
List forces: gravity (down) and magnetic (unknown). No tension or normal force acts.
Recall the Lorentz force expression and its dependence on speed and field.
Sketch \( \mathbf{v} \) west, choose \( \mathbf{B} \) south, verify \( \mathbf{v}\times\mathbf{B} \) points up.
Set \(q = 1\;\text{C}\) mentally to see how speed scales with charge.
Struggle is normal! Try to solve on your own before checking the hints.
LCR Circuit Surprise
In a series LCR circuit \(V_R = V_C = V_L = 10\,\text{V}\). The capacitor is short-circuited. What is the new rms voltage across the inductor?
Equal voltages on \(R, L, C\) indicate the circuit is at resonance.
At resonance, \(V_{\text{supply}} = V_R = 10\text{ V}\). So \(I = 10 / R\) and \(X_L = R\).
With \(C\) shorted, \(Z = \sqrt{R^{2}+X_L^{2}} = R\sqrt{2}\). New \(I = 10/(R\sqrt{2})\). Hence \(V_L = I X_L = 10/\sqrt{2} \approx 7.1\text{ V}\).
First decide what resonance tells you about \(X_L\) and \(X_C\).
Recall impedance triangles to combine \(R\) and \(X_L\).
Sketch phasors for \(V_R, V_L, V_C\) before and after removing \(C\).
Try \(R = 10\,\Omega, X_L = 10\,\Omega\) numerically to verify the formula.
Struggle is normal! Try to solve on your own before checking the hints.
Wave Optics – Young’s Double-Slit
Light of 400 nm and 600 nm passes through a double-slit. How far from the central maximum will the first common dark fringe appear?
Diagram not required for this calculation.
Write the dark-band condition for each colour, then set the path differences equal.
Assume \( (m+\tfrac12)\lambda_{400}=m\lambda_{600} \). Solve for the smallest positive integer \( m \).
You get \( m=1 \), so \( \delta =600\text{ nm} \). Insert this into \( y=\delta D/d \) for the required distance.
Handle each wavelength separately, then combine results.
Remember bright-overlap rules; here add the half-order shift for darkness.
Sketch both fringe sets; mark where the first overlap vanishes.
Try λ ratio 1 : 2 to see the pattern before tackling 400 : 600 nm.
Struggle is normal! Try to solve on your own before checking the hints.
Fission vs Fusion Decision
On the binding-energy per nucleon graph, points W(190), X(90), Y(60) and Z(30) are marked. Which nucleus can release energy by fission and which by fusion? Give a brief reason.
Binding energy per nucleon vs mass number (schematic)
First, see how far each A value lies from the peak around 60.
Heavy nuclei to the right split; very light nuclei to the left combine—both moves aim for A ≈ 60.
W(190) can increase B.E./A by splitting into fragments near 90 → fission. Z(30) can gain B.E./A by joining another light nucleus to reach ~60 → fusion.
Order the four A values, then compare each with 60.
Recall that iron-nickel are most stable due to highest B.E./A.
Sketch the B.E./A curve and plot W, X, Y, Z.
Think of uranium fission and hydrogen fusion as extreme examples.
Struggle is normal! Try to solve on your own before checking the hints.
CBSE Grade 12 Physics
Parallel-plate capacitor: plates area \(A\), air gap \(d\). Case 1 – dielectric slab thickness \(t\), permittivity \(\varepsilon_r\). Case 2 – metal slab thickness \(t<d\). Derive capacitances \(C_1, C_2\) and decide which is larger.
Treat the slab and remaining air as two capacitors in series.
Write \(V=E_1 t + E_2(d-t)\) and substitute \(E=\sigma/\varepsilon\).
Obtain \(C_1=\frac{\varepsilon_0 A}{d - t + t/\varepsilon_r}\). For the metal slab \(E=0\) inside, so \(C_2=\frac{\varepsilon_0 A}{d-t}\). Compare denominators.
Separate the problem into slab region and air region.
Remember electric field behaviour inside conductors and dielectrics.
Draw a side view labelling \(t\), \(d-t\), and field directions.
Check results for \(t=0\) or \(\varepsilon_r=1\) to build confidence.
Struggle is normal! Try to solve on your own before checking the hints.
Field Inside a Current-Carrying Wire
For a long solid wire of radius \(a\) carrying uniform current \(I\), find the ratio \(B_{\text{above}}:B_{\text{below}}\) where “above” is \(\frac{a}{2}\) outside the surface and “below” is \(\frac{a}{2}\) inside the surface.
No diagram required
Identify whether each point lies inside or outside the wire by calculating its distance from the axis.
Use \(B(r)=\frac{\mu_{0} I r}{2\pi a^{2}}\) for \(r=\frac{a}{2}\) and \(B(r)=\frac{\mu_{0} I}{2\pi r}\) for \(r=\frac{3a}{2}\).
Compute \(B_{\text{below}}=\frac{\mu_{0}I}{2\pi a^{2}}\cdot\frac{a}{2}\) and \(B_{\text{above}}=\frac{\mu_{0}I}{2\pi}\cdot\frac{2}{3a}\). Then form the ratio.
Draw the wire cross-section, label \(r=\frac{a}{2}\) and \(r=\frac{3a}{2}\).
Recall that inside a uniformly current-filled region \(B\propto r\); outside \(B\propto 1/r\).
Sketch concentric circular field lines with varying spacing inside and outside the wire.
Evaluate \(B\) at the centre and at the surface to verify you are using the correct formula.
Struggle is normal! Try to solve on your own before checking the hints.
EM Spectrum (Grade 12 Physics)
Match each electromagnetic wave with its usual production mechanism.
1. Radio waves a) Rapid oscillation of conduction electrons in an aerial
2. Microwaves b) Klystron / magnetron valve
3. Infra-red c) Vibrations of atoms & molecules in matter
4. Visible light d) Electronic transitions within atoms
Write the correct 1-a, 2-b … pairs.
Start with the extremes: radio waves come from antenna currents.
Think of the device that powers radar and microwave ovens—the klystron/magnetron.
Map now: conduction electrons → radio, vacuum tube → microwave, molecular vibration → IR, atomic transition → visible.
List the four mechanisms, then match one wave at a time.
Recall how your radio and microwave oven generate waves.
Sketch the EM spectrum and label each source.
If you only knew radio waves, what mechanism might the next higher band use?
Struggle is normal! Try to solve on your own before checking the hints.
Decoding Photoelectric Curves
Three photoelectric I–V curves A, B and C are recorded with different monochromatic lights on the same metal. For every pair (A,B), (A,C) and (B,C), state whether the two lights share intensity, frequency or neither, and justify from the curves.
Curve sketch goes here if provided
Match curves whose plateaus reach the same current; those beams have identical intensity.
Equal stopping potentials mean equal photon energy, hence same frequency.
Identify pairs with matching plateau → same intensity; matching intercept → same frequency. If neither matches, both differ.
Examine current plateau and cutoff voltage separately before combining clues.
Recall Einstein’s explanation linking photon energy to electron kinetic energy.
Sketch vertical lines from each plateau to see overlaps quickly.
Imagine two identical lamps with different filters to predict graph changes.
Struggle is normal! Try to solve on your own before checking the hints.
Grade 12 Physics | Rectification
In the AC → X → Y → DC block, name X and Y. Sketch the voltage after each stage. How will the DC waveform change if the transformer’s centre-tap moves closer to \(D_1\)?
First, identify what lowers AC voltage before diodes take over.
X = step-down transformer. Y = full-wave rectifier followed by a smoothing capacitor.
Draw sine after X. After Y, both half-cycles become positive (pulsating DC). Moving the tap toward \(D_1\) enlarges one half-cycle and shifts average DC upward, adding ripple.
Match each block to its role: transform, rectify, filter.
Recall lab work on bridge and centre-tap rectifiers.
Sketch voltage across the load after each stage.
Assume ideal diodes and equal halves before considering tap shift.
Current Electricity – Network Analysis
A uniform wire of total resistance 12 Ω is bent into a circle. A 10 Ω resistor joins the opposite points C and D. A battery of emf 8 V is connected across another pair of opposite points A and B. Determine the current through the arc A → D.
Sketch the equivalent Wheatstone bridge on your notepad.
Think of the circle as two equal 6 Ω semicircular arcs between A–C–B and A–D–B.
Redraw the arrangement as a Wheatstone bridge where the 10 Ω resistor is the bridge arm CD.
Apply Kirchhoff’s loop law to two independent loops or test for bridge balance, then solve for branch currents without yet computing the final numeric answer.
Convert the circular layout into a four-resistor Wheatstone bridge diagram.
Recall that equal opposite arms can balance a bridge, potentially nullifying current through the 10 Ω path.
Label currents in each branch and mark assumed directions before writing \( \sum V = 0 \) equations.
Imagine removing the 10 Ω resistor; predict current split, then re-introduce it to see the change.
Struggle is normal! Try to solve on your own before checking the hints.
Grade 12 Physics – CBSE
A coil with \(N\) turns and area \(A\) rotates at angular speed \( \omega \) in a uniform magnetic field \(B\). Using Faraday’s law, derive the instantaneous emf \( \varepsilon = N A B \omega \sin \omega t \). Also state the practical source of this electrical energy.
No diagram provided
Express the magnetic flux as \( \Phi = B A \cos (\omega t) \).
Differentiate \( \Phi \) with respect to time and apply Faraday’s law: \( \varepsilon = -\dfrac{d\Phi}{dt} \).
You should arrive at \( \varepsilon = N A B \omega \sin \omega t \) with peak value \( \varepsilon_0 = N A B \omega \). In real generators, mechanical work from turbines supplies the energy.
First write flux, then differentiate—two clear steps.
Recall Faraday’s and Lenz’s laws determine magnitude and sign.
Picture the coil’s plane sweeping through the magnetic field lines.
Try one loop (\(N=1\)) to confirm the sinusoidal nature of \( \varepsilon \).
Struggle is normal! Try to solve on your own before checking the hints.
Ray Optics – Prism
A right-angled prism (\(C = 45^{\circ}\)) receives a ray as shown. Side AC is immersed in a liquid of refractive index \(n = \frac{2}{\sqrt{3}}\). Will the emerging ray graze, refract, or undergo total internal reflection? Draw its path.
[Diagram as given in paper]
Recall the prism’s refractive index you found earlier when the ray just grazed in air.
Compute new critical angle at AC: \(\sin C = \dfrac{n_{\text{liquid}}}{n_{\text{prism}}}\).
Compare \(45^{\circ}\) with the critical angle. If \(45^{\circ}\) < \(C\), TIR; if equal, grazing; if >, refraction into liquid.
Calculate critical angle first, then decide the ray’s fate.
You earlier assumed air outside—update that step for liquid.
Draw normals at AC and mark incident \(45^{\circ}\) angle.
Imagine liquid is air to see why outcome changes.
Struggle is normal! Try to solve on your own before checking the hints.
Grade 12 Physics – Bohr Model
Hydrogen has only one electron. Why does its emission spectrum still show many discrete lines?
Energy-level diagram could be sketched here
Consider how many hydrogen atoms are present in a glowing sample.
Different atoms can have their lone electron in different excited states at the same time.
Each occupied excited level \(n_i\) can decay through several lower levels \(n_f\). Every allowed transition emits a photon with a unique energy, producing multiple spectral lines.
List energy levels, then count possible downward jumps.
Recall the Balmer lines and their level diagram.
Sketch Bohr levels and draw arrows for transitions.
Imagine only two levels and observe how one line appears.
Struggle is normal! Try to solve on your own before checking the hints.
Quick recap: use symmetry with Gauss’s law and Ampère’s rule to write fields instantly.
Remember: at resonance current peaks as \(X_L = X_C\); reactances switch sign beyond this point.
Dark fringes shift for two colours; recall \(d\sin\theta=(m+1/2)\lambda\) separately.
Remember: nuclei are most stable at \(A \approx 60\); fusion below and fission above release energy.
Recap power-supply sequence: transformer → rectifier → filter conditions voltage for circuits.
Thing to remember: sketch and label angles before equations; clarity prevents sign errors.