FAD1022: Max Score Strategy — Minimal Study
[!tip] The Goal Score ~129/129 by picking the RIGHT questions and studying ONLY the topics you'll actually answer.
Total formulas to memorise: ~18 Total study time: 2–3 hours
The Maths
| Section | Format | Marks | Your Pick |
|---|---|---|---|
| A | 15 structured × 3 (all compulsory) | 45 | All 15 |
| B | 4 Q → pick 3 × 12 | 36 | B2 + B1 + B3 ✅ |
| C | 6 Q → pick 4 × 12 | 48 | C2 + C3 + C5 + C6 ✅ |
| Total attempted | 129 |
Section A — Structured Questions (all compulsory, 45 marks)
A1: Capacitor Charging & Discharging
- Charging:
- $$q(t) = Q(1 - e^{-t/\tau})$$
- $$i(t) = \frac{V}{R}e^{-t/\tau}$$
- $$V_C(t) = V(1 - e^{-t/\tau})$$
- Discharging:
- $$q(t) = Q_0 e^{-t/\tau}$$
- $$i(t) = -I_0 e^{-t/\tau}$$
- $$V_C(t) = V_0 e^{-t/\tau}$$
- Time constant: $$\tau = RC$$
- Key graph shapes:
- Charging: exponential rise to Q (asymptotic)
- Discharging: exponential decay to 0
- At $t = \tau$: charging reaches ~63% of final value; discharging falls to ~37% of initial
A2: Kirchhoff's Current Law
- $$\sum I_{in} = \sum I_{out}$$ at any junction
- Equivalent: $$\sum I = 0$$ (currents entering positive, leaving negative)
- Simple conservation of charge — currents entering a node must equal currents leaving it
- Typical Section A: given two currents entering and one leaving, find the missing current
A3: Amplifier Formulas
- Inverting:
- $$V_{out} = -\frac{R_f}{R_{in}} V_{in}$$
- Negative sign means 180° phase shift
- Non-inverting:
- $$V_{out} = \left(1 + \frac{R_f}{R_{in}}\right) V_{in}$$
- Positive gain, no phase shift
- Voltage follower (non-inverting special case, no feedback resistors): $$V_{out} = V_{in}$$
- Just memorise these two formulas — plug and chug
A4: Ampere's Law — Inside Wire (r < R)
- Formula:
- $$B(r) = \frac{\mu_0 I r}{2\pi R^2}$$
- Derivation for Section A:
- $$\oint \vec{B} \cdot d\vec{l} = B(2\pi r) = \mu_0 I_{enc}$$
- $$I_{enc} = I \cdot \frac{\pi r^2}{\pi R^2} = I\frac{r^2}{R^2}$$
- ∴ $$B(2\pi r) = \mu_0 I \frac{r^2}{R^2} \implies B = \frac{\mu_0 I r}{2\pi R^2}$$
- Check: at r = R, $$B = \frac{\mu_0 I}{2\pi R}$$ which matches the outside-wire formula
A5: Lenz Law
- 🚫 NOT TESTED — skip entirely
Section B — Pick 3 of 4 (36 marks)
✅ PICK B2: Capacitor + Dielectric + DC
Parts a & b: Capacitance & Energy
- Parallel plate capacitance:
- $$C = \kappa\varepsilon_0 \frac{A}{d}$$
- $\kappa$ = dielectric constant (1 for vacuum/air)
- Energy stored:
- $$U = \frac12 CV^2 = \frac12 QV = \frac{Q^2}{2C}$$
- Dielectric effects:
- Battery connected (V constant): inserting dielectric → C↑ (×κ), Q↑ (×κ), U↑ (×κ)
- Battery disconnected (Q constant): inserting dielectric → C↑ (×κ), V↓ (÷κ), U↓ (÷κ)
- Removing dielectric reverses the effect in each case
Part c: Voltage Divider (Loaded & Unloaded)
- Unloaded:
- $$V_{out} = V_{in} \frac{R_2}{R_1 + R_2}$$
- Loaded (with $R_L$ across $R_2$):
- $$R_{parallel} = \frac{R_2 R_L}{R_2 + R_L}$$
- $$V_{out} = V_{in} \frac{R_{parallel}}{R_1 + R_{parallel}}$$
- Loading effect: Adding a load reduces $V_{out}$ compared to the unloaded value — the smaller $R_L$, the more severe the loading
- Rule of thumb: To minimise loading, make $R_L \gg R_2$
✅ PICK B1: Electrostatic — E-field & Projectile Motion
E-field Vector
- Point charge:
- $$\vec{E} = \frac{kQ}{r^2} \hat{r}$$
- $k = \frac{1}{4\pi\varepsilon_0} = 8.99 \times 10^9\ \text{N·m}^2/\text{C}^2$
- Force on test charge:
- $$\vec{F} = q\vec{E}$$
- Superposition principle:
- $$\vec{E}_{net} = \sum \vec{E}_i$$
- Add fields as vectors (resolve x and y components)
Projectile Motion in E-field
- Setup: Charge q enters uniform E-field between parallel plates with initial horizontal velocity v₀
- Vertical acceleration:
- $$a_y = \frac{F}{m} = \frac{qE}{m}$$
- Time in field:
- $$t = \frac{L}{v_0}$$ where L = plate length
- Vertical deflection at exit:
- $$y = \frac12 a_y t^2 = \frac12 \cdot \frac{qE}{m} \cdot \left(\frac{L}{v_0}\right)^2$$
- Exit velocity components:
- $v_x = v_0$ (constant, no horizontal force)
- $v_y = a_y t = \frac{qE}{m} \cdot \frac{L}{v_0}$
- Exit angle:
- $$\tan\theta = \frac{v_y}{v_x} = \frac{qEL}{mv_0^2}$$
- Analogy: treat like gravity projectile but with $a_y = qE/m$ instead of g
✅ PICK B3: AC (PRC + PLC + PCC)
Phasor Diagrams
- Resistive (PRC): V and I in phase (0° phase difference)
- Inductive (PLC): Voltage leads current by 90° (V ahead of I)
- Capacitive (PCC): Current leads voltage by 90° (I ahead of V)
- CIVIL mnemonic:
- C — I leads V
- V leads I — L
Power Types
| Power | Symbol | Formula | Unit | Description |
|---|---|---|---|---|
| Real/Active (PRC) | P | $V_{rms}I_{rms}\cos\phi$ | W (watts) | Dissipated by resistor |
| Inductive Reactive (PLC) | Q_L | $V_{rms}I_{rms}\sin\phi$ | VAR | Stored/released by inductor |
| Capacitive Reactive (PCC) | Q_C | $V_{rms}I_{rms}\sin\phi$ | VAR | Stored/released by capacitor |
| Apparent | S | $V_{rms}I_{rms}$ | VA | Total power supplied |
- Power Triangle:
- $$S^2 = P^2 + (Q_L - Q_C)^2$$
- Power Factor:
- $$\cos\phi = \frac{P}{S} = \frac{R}{Z}$$
- Power factor = 1 → purely resistive (maximum real power)
- Power factor = 0 → purely reactive (no real power dissipation)
RLC Series Circuit
- Impedance:
- $$Z = \sqrt{R^2 + (X_L - X_C)^2}$$
- $X_L = \omega L$ (inductive reactance)
- $X_C = \frac{1}{\omega C}$ (capacitive reactance)
- Phase angle:
- $$\phi = \tan^{-1}\left(\frac{X_L - X_C}{R}\right)$$
- Interpretation:
- $X_L > X_C$ → positive φ → inductive → V leads I
- $X_C > X_L$ → negative φ → capacitive → I leads V
- $X_L = X_C$ → resonance → φ = 0 → purely resistive
❌ SKIP B4: AC Claims & RLC
Conceptual questions about identifying true/false statements. Requires precise judgement on edge cases. Trickier mark allocation and more ambiguous than the formulaic B1-B3. Not worth the study time.
Section C — Pick 4 of 6 (48 marks)
✅ PICK C2: EM — AC Motor Torque
Single formula, extended across parts:
- $$\tau = NIAB\sin\theta$$
- N = number of turns in the coil
- I = current through the coil
- A = area of the loop ($A = l \times w$)
- B = uniform magnetic field strength
- $\theta$ = angle between B-field and normal to the loop's plane
- Maximum torque:
- Occurs at $\theta = 90^\circ$ (plane of loop parallel to B-field)
- $$\tau_{max} = NIAB$$
- Minimum torque:
- Occurs at $\theta = 0^\circ$ (plane of loop perpendicular to B-field)
- $$\tau = 0$$ — forces are colinear, no turning effect
- Magnetic dipole moment:
- $$\vec{\mu} = NIA\ \hat{n}$$ where $\hat{n}$ is normal to the loop
- Alternative: $$\tau = \mu B \sin\theta$$
- AC motor behaviour:
- Current alternates → torque varies sinusoidally with time
- Average torque is non-zero → continuous rotation
- Direction: Use Fleming's Left-Hand Rule (thumb = motion, index = field, middle = current)
✅ PICK C3: Transformer — Self & Mutual Induction
Self-Inductance
- Definition:
- $$L = \frac{N\Phi}{I}$$
- Units: Henry (H)
- Solenoid:
- $$L = \frac{\mu_0 N^2 A}{\ell}$$
- $\ell$ = length of solenoid, A = cross-sectional area
- Back EMF:
- $$\mathcal{E} = -L\frac{dI}{dt}$$
- Negative sign from Lenz Law (opposes change)
- Energy stored in inductor:
- $$U = \frac12 LI^2$$
Mutual Inductance
- Definition:
- $$M = \frac{N_2\Phi_{21}}{I_1} = \frac{N_1\Phi_{12}}{I_2}$$
- With coupling coefficient:
- $$M = k\sqrt{L_1 L_2}$$
- k = 1 for perfect coupling (all flux links both coils)
- k = 0 for no coupling
- Reciprocity:
- $$M_{12} = M_{21} = M$$
Transformer
- Turns ratio (voltage):
- $$\frac{V_s}{V_p} = \frac{N_s}{N_p}$$
- Current ratio:
- $$\frac{I_s}{I_p} = \frac{N_p}{N_s}$$
- Step-up: $N_s > N_p$ → $V_s > V_p$, $I_s < I_p$
- Step-down: $N_s < N_p$ → $V_s < V_p$, $I_s > I_p$
- Ideal transformer (power conserved):
- $$V_p I_p = V_s I_s$$
- $$P_{in} = P_{out}$$ (negligible losses)
- Transformer equation:
- $$\frac{V_p}{N_p} = \frac{V_s}{N_s}$$ (volts per turn is constant)
✅ PICK C5: Atomic — Bohr Radius Derivation
Step-by-step derivation (memorise the flow):
Step 1: Coulomb attraction = centripetal force $$\frac{ke^2}{r^2} = \frac{mv^2}{r}$$
Step 2: Angular momentum is quantised $$mvr = n\hbar \quad \text{where } \hbar = \frac{h}{2\pi}$$
Step 3: From Step 1: $$mv^2 = \frac{ke^2}{r}$$
Step 4: From Step 2: $$v = \frac{n\hbar}{mr}$$
Step 5: Substitute v into Step 3: $$m\left(\frac{n\hbar}{mr}\right)^2 = \frac{ke^2}{r} \quad\implies\quad \frac{n^2\hbar^2}{mr^2} = \frac{ke^2}{r}$$
Step 6: Solve for r: $$r_n = \frac{n^2\hbar^2}{mke^2} = n^2 a_0$$ where $$a_0 = \frac{\hbar^2}{mke^2} = 0.529\ \text{Å}$$ (Bohr radius)
Energy Levels
- Total energy: $$E_n = \frac12 mv^2 - \frac{ke^2}{r} = -\frac{ke^2}{2r}$$
- Substitute $r_n$: $$E_n = -\frac{ke^2}{2a_0} \cdot \frac{1}{n^2} = -\frac{13.6\ \text{eV}}{n^2}$$
- Ground state (n = 1): E₁ = -13.6 eV
- Ionisation energy: 13.6 eV (energy to remove electron from ground state)
- Transition energy: $$\Delta E = E_f - E_i = 13.6\left(\frac{1}{n_i^2} - \frac{1}{n_f^2}\right) \text{eV}$$
- Wavelength: $$\lambda = \frac{hc}{\Delta E} = \frac{1240\ \text{eV·nm}}{\Delta E\ (\text{in eV})}$$
Spectral Series
| Series | n_f | Region | First line (n_i→n_f) |
|---|---|---|---|
| Lyman | 1 | UV | 2 → 1 (121.6 nm) |
| Balmer | 2 | Visible | 3 → 2 (656.3 nm) |
| Paschen | 3 | Infrared | 4 → 3 (1875 nm) |
✅ PICK C6: Photoelectric Effect
Key Equations
- Photon energy:
$$E = hf = \frac{hc}{\lambda}$$
- h = 6.626 × 10⁻³⁴ J·s (Planck's constant)
- c = 3.0 × 10⁸ m/s
- hc = 1240 eV·nm (useful shortcut)
- Einstein's photoelectric equation:
$$K_{max} = hf - \phi$$
- $K_{max}$ = maximum kinetic energy of ejected electrons
- $\phi$ = work function of the metal (minimum energy to eject)
- Stopping potential:
$$eV_s = K_{max} \quad\implies\quad V_s = \frac{hf - \phi}{e}$$
- $V_s$ = potential needed to stop the most energetic electrons
- Threshold frequency: $$f_0 = \frac{\phi}{h} \quad (\text{when } K_{max} = 0)$$
- Cutoff wavelength: $$\lambda_c = \frac{hc}{\phi}$$
- Maximum electron speed:
$$v_{max} = \sqrt{\frac{2K_{max}}{m_e}}$$
- $m_e = 9.11 \times 10^{-31}$ kg
Graphs
- $K_{max}$ vs $f$:
- Straight line: slope = h (Planck's constant)
- y-intercept = -φ (negative work function)
- x-intercept = f₀ (threshold frequency)
- $V_s$ vs $f$:
- Straight line: slope = h/e
- y-intercept = -φ/e
- Effect of increasing intensity:
- Doubles photocurrent (more photons → more electrons)
- Does NOT change $K_{max}$ or $V_s$
- Effect of higher work function:
- Graph shifts right (higher f₀)
- Graph shifts down (more negative intercept)
Past Year Pattern (from leak)
| Part | Typical Question | Marks |
|---|---|---|
| (a) | Define terms / state Einstein's equation | 2–3 |
| (b) | Calculate $K_{max}$, $V_s$, $v_{max}$, or $\lambda$ | 5–6 |
| (c) | Sketch graph, label axes, explain effect of changing parameters | 3–4 |
❌ SKIP — These Questions (Don't Study)
| Question | Why Skip |
|---|---|
| A5 (Lenz Law) | Explicitly NOT TESTED per leak |
| B4 (AC Claims) | Tricky conceptual true/false; ambiguous marking |
| C1 (Magnetism — Gauss & Ampere, 4-wire) | Heaviest derivation in the paper; too much time |
| C4 (Semi & Biasing) | Many sub-parts; clipper circuits need specialised practice |
Quick Reference: All Formulas You Need
| # | Topic | Formula | Notes |
|---|---|---|---|
| 1 | Capacitance | $$C = \kappa\varepsilon_0 \frac{A}{d}$$ | Parallel plate |
| 2 | Capacitor energy | $$U = \frac12 CV^2 = \frac{Q^2}{2C}$$ | Pick the convenient form |
| 3 | RC charging | $$q(t) = Q(1-e^{-t/\tau})$$ | $\tau = RC$ |
| 4 | RC discharging | $$q(t) = Q_0 e^{-t/\tau}$$ | |
| 5 | Voltage divider | $$V_{out} = V_{in}\frac{R_2}{R_1+R_2}$$ | Unloaded |
| 6 | Voltage divider (loaded) | $$V_{out} = V_{in}\frac{R_{eq}}{R_1+R_{eq}}$$ | $R_{eq} = R_2 \parallel R_L$ |
| 7 | E-field | $$\vec{E} = \frac{kQ}{r^2} \hat{r}$$ | $k = 1/4\pi\varepsilon_0$ |
| 8 | Acceleration in E-field | $$a_y = \frac{qE}{m}$$ | Analogy: gravity but with qE/m |
| 9 | Deflection in E-field | $$y = \frac12 \frac{qE}{m} \left(\frac{L}{v_0}\right)^2$$ | |
| 10 | Amplifier (inverting) | $$V_{out} = -\frac{R_f}{R_{in}}V_{in}$$ | 180° phase shift |
| 11 | Amplifier (non-inv) | $$V_{out} = \left(1+\frac{R_f}{R_{in}}\right)V_{in}$$ | No phase shift |
| 12 | Ampere inside wire | $$B = \frac{\mu_0 I r}{2\pi R^2}$$ | r < R |
| 13 | Power triangle | $$S^2 = P^2 + (Q_L - Q_C)^2$$ | $\cos\phi = P/S$ |
| 14 | Motor torque | $$\tau = NIAB\sin\theta$$ | Max at 90° |
| 15 | Self-inductance | $$L = \frac{\mu_0 N^2 A}{\ell}$$ | Solenoid |
| 16 | Transformer | $$\frac{V_s}{V_p} = \frac{N_s}{N_p}$$ | Also $I_s/I_p = N_p/N_s$ |
| 17 | Bohr radius | $$r_n = n^2 a_0$$ | $a_0 = 0.529\ \text{Å}$ |
| 18 | Bohr energy | $$E_n = -\frac{13.6}{n^2}\ \text{eV}$$ | Ionisation = 13.6 eV |
| 19 | Photoelectric | $$K_{max} = hf - \phi$$ | |
| 20 | Stopping potential | $$eV_s = K_{max}$$ |
Study Order (highest yield first)
| Step | Topic | Time | Rationale |
|---|---|---|---|
| 1 | B2 formulas — capacitance + voltage divider | 15 min | High marks, few formulas, formulaic |
| 2 | C6 formulas — photoelectric equation + graphs | 15 min | 3-part pattern repeats yearly |
| 3 | C2 formula — motor torque | 5 min | Single formula → 12 marks |
| 4 | C3 formulas — transformer ratios + inductance | 15 min | Turns ratio is plug-and-chug |
| 5 | C5 derivation — Bohr radius + energy levels | 20 min | Step-by-step → full derivation marks |
| 6 | B1 formulas — E-field + projectile kinematics | 15 min | Standard mechanics with E-field |
| 7 | B3 formulas — power triangle + phasors | 15 min | CIVIL mnemonic + 3 equations |
| 8 | A formulas — quick-fire revision | 20 min | All compulsory, covers all topics |
| 9 | Targeted drill pack — apply everything | 60 min | FAD1022 Rapid-Fire Drill — Leak Topics |
| Total | ~3 hours |