ESAT Worked Solutions · Physics
ESAT Paper 1 Physics Worked Solutions
Complete step-by-step worked solutions. Part of the ESAT preparation guide.
Question 1
Back to top ↑A portable generator works by manually turning a hand crank to produce power. The generator has a mechanical efficiency of 80%. The crank has a radius of $25 \ \text{cm}$ and the operator can spin it with a force of $100 \ \text{N}$. At what speed must they turn it to power a $100 \ \text{W}$ bulb? Assume any electrical losses are negligible.
Key Idea (💡): Electrical bulb requires $P_{\text{out}} = 100$ W. Efficiency $\eta = 80 \% = 0.80 \implies P_{\text{in}} = \frac{100}{0.80} = 125$ W. Torque $\tau = F \cdot r = 100 \cdot 0.25 = 25$ N m. Angular speed $\omega = \frac{P_{\text{in}}}{\tau} = \frac{125}{25} = 5.00$ rad/s.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. 5.00 radians/second
Fastest Approach (🚀):
Efficiency equation: $P_{\text{out}} = \eta \cdot P_{\text{in}} \implies 100 = 0.80 \cdot P_{\text{in}} \implies P_{\text{in}} = 125 \ \text{W}$.
Torque $\tau = F \cdot r = 100 \times 0.25 = 25 \text{N m}$.
Rotational power $P_{\text{in}} = \tau \omega \implies 125 = 25 \omega \implies \omega = 5.00\ \text{rad/s}$.
Matches Option D.
Step-by-Step Breakdown:
1. Rotational Mechanics & Efficiency Principles
A. Mechanical Efficiency Law
$\eta = \frac{P_{\text{out}}}{P_{\text{in}}} \implies P_{\text{in}} = \frac{P_{\text{out}}}{\eta}$
B. Rotational Torque Formula
$\tau = F \cdot r$
C. Rotational Power Formula
$P_{\text{mechanical}} = \tau \cdot \omega \quad (\omega \text{in rad/s})$
2. System Parameters & Input Power Calculation
- Electrical output required: $P_{\text{out}} = 100 \ \text{W}$.
- Mechanical efficiency: $\eta = 80 \% = 0.80$.
- Mechanical input power required:
$P_{\text{in}} = \frac{100 \ \text{W}}{0.80} = 125 \ \text{W}$
3. Torque & Angular Speed Calculation
- Force applied: $F = 100 \ \text{N}$. Radius: $r = 25 \ \text{cm} = 0.25 \ \text{m}$.
- Torque generated: $\tau = 100 \times 0.25 = 25 \text{N m}$.
- Solve for angular velocity $\omega$:
$P_{\text{in}} = \tau \cdot \omega \implies 125 = 25 \cdot \omega \implies \omega = \frac{125}{25} = 5.00\ \text{rad/s}$
4. Option Matching
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. 0.51 radians/second — Incomplete Calculation
Failing to account for mechanical efficiency. - B. 77 radians/second — Misapplied Formula
Multiplying by the efficiency instead of dividing to find input power. - C. 36 radians/second — Unit Conversion Error
Using the diameter instead of the radius for the torque calculation. - E. 2 radians/second — Conceptual Misunderstanding
Dividing by the efficiency twice.
Common Mistake (⚠️):
Forgetting to account for efficiency or applying it backward by multiplying $100 \ \text{W}$ by 0.8 instead of dividing.
Takeaway (📌):
Always apply efficiency to the input power side of the energy conservation equation.
Question 2
Back to top ↑A cylindrical piece of wire with resistance $2.0 \ \Omega$ and radius $1 \ \text{cm}$, is connected to a $6 \ \text{V}$ battery. If the radius of the wire is doubled, how many electrons will flow through it every second? The charge of an electron is $1.6 \times 10^{-19}C$.
Key Idea (💡): Doubling the radius of a cylindrical wire increases its cross sectional area by a factor of four, which divides its resistance by four.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. $7.5\times10^{19}$
Fastest Approach (🚀):
Original resistance $R_0 = 2.0\ \Omega$.
Doubling radius increases area by 4, so new resistance is $R = 2.0 / 4 = 0.5\ \Omega$.
Ohm's law: $I = V / R = 6 / 0.5 = 12 \ \text{A} = 12 \text{C/s}$.
Number of electrons: $N = \frac{12}{1.6 \times 10^{-19}} = 7.5 \times 10^{19}\ \text{electrons/sec}$.
Matches Option C.
Step-by-Step Breakdown:
1. Resistivity, Ohm's Law & Charge Quantization Principles
A. Pouillet's Resistivity Law
$R = \rho \frac{L}{A} = \frac{\rho L}{\pi r^2}$
B. Ohm's Law
$I = \frac{V}{R}$
C. Charge Quantization Law
$I = \frac{\Delta Q}{\Delta t} = N \cdot e \quad (e = 1.6 \times 10^{-19}C)$
2. Resistance Scaling with Wire Radius
- Original resistance $R_0 = 2.0\ \Omega$. Radius $r_0 = 1$ cm.
- Doubling radius $r_1 = 2r_0 \implies A_1 = \pi(2r_0)^2 = 4\pi r_0^2 = 4A_0$.
- New resistance:
$R_{\text{new}} = \frac{R_0}{4} = \frac{2.0}{4} = 0.5\ \Omega$
3. Current & Electron Flow Calculation
- Voltage $V = 6 \ \text{V}$.
- New current: $I = \frac{6}{0.5} = 12 \ \text{A} = 12 \text{C/s}$.
- Number of electrons per second $N$:
$N = \frac{I}{e} = \frac{12}{1.6 \times 10^{-19}} = 7.5 \times 10^{19}\ \text{electrons/second}$
4. Option Matching
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. $1.9\times10^{19}$ — Unit Conversion Error
Assuming resistance is inversely proportional to radius rather than area. - B. $3.8\times10^{19}$ — Unit Conversion Error
Forgetting to halve the resistance when the radius doubles. - D. $1.5\times10^{20}$ — Unit Conversion Error
Squaring the current instead of simply dividing by the charge. - E. $4.7 \times 10^{20}$ — Unit Conversion Error
Using the wrong charge constant or making a power of 10 order-of-magnitude error.
Common Mistake (⚠️):
Assuming resistance is inversely proportional to radius rather than the square of the radius.
Takeaway (📌):
When a wire's radius changes by a factor of $x$, its resistance changes by a factor of $1/\text{x^2}$.
Question 3
Back to top ↑The amount of solar radiation that reaches the Earth which is reflected is called the albedo factor, $a$. The incident solar radiation flux per unit area at the Earth is $\Omega$ and the Stefan-Boltzmann constant is $\sigma$. Which of the following expressions represents the black-body temperature of the Earth's surface, $T_s$, in terms of $\Omega$, $\sigma$ and $a$?
Key Idea (💡): The Earth must radiate exactly as much power as it absorbs to maintain a stable black body temperature.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. $\sqrt[4]{\Omega(1-a)/\sigma}$
Fastest Approach (🚀):
Absorbed radiation fraction: $(1 - a)$. Total absorbed power $= \Omega(1 - a)$.
Stefan-Boltzmann law: $P = \sigma T_s^4$.
Equate: $\sigma T_s^4 = \Omega(1 - a) \implies T_s = \sqrt[4]{\frac{\Omega(1-a)}{\sigma}}$.
Matches Option B.
Step-by-Step Breakdown:
1. Stefan-Boltzmann Law & Albedo Definitions
A. Albedo Factor ($a$)
The fraction of incident radiation reflected by a body. The absorbed fraction is $(1 - a)$.
B. Stefan-Boltzmann Law
Power emitted per unit surface area by a black body at temperature $T$ is $P = \sigma T^4$, where $\sigma$ is the Stefan-Boltzmann constant.
C. Radiative Equilibrium Principle
$\text{Absorbed Flux} = \text{Emitted Flux}$
2. Energy Conservation Balance
- Incoming solar radiation $= \Omega$.
- Reflected flux $= a \Omega \implies$ Absorbed flux $= \Omega(1 - a)$.
- Emitted thermal black-body flux $= \sigma T_s^4$.
3. Solving for Surface Temperature $T_s$
$\sigma T_s^4 = \Omega(1 - a)$
$T_s^4 = \frac{\Omega(1 - a)}{\sigma}$
$T_s = \sqrt[4]{\frac{\Omega(1 - a)}{\sigma}}$
4. Option Matching
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. $\sqrt[4]{\Omega(a-1)/\sigma}$ — Sign Error
Inverting the absorption fraction to (a-1), which incorrectly gives a negative value. - C. $\sqrt[4]{\Omega(a-1)}$ — Misapplied Formula
Forgetting to divide by the Stefan-Boltzmann constant in the formula. - D. $\sqrt[4]{\Omega(1-a)}$ — Misapplied Formula
Forgetting to divide by the Stefan-Boltzmann constant in the final rearranged formula. - E. $\sqrt[4]{\Omega/\sigma}$ — Conceptual Misunderstanding
Ignoring the albedo factor completely and assuming 100% absorption.
Common Mistake (⚠️):
Using the albedo factor $a$ as the absorbed fraction rather than the reflected fraction.
Takeaway (📌):
Albedo represents reflectivity, so always use $(1 - \text{albedo})$ for energy absorption.
Question 4
Back to top ↑Waves are generated as a rope held from a point $P$ is vibrated vertically. The wavelength of the waves is $1.2 \ \text{m}$ and they travel along rope at a speed of $2.4 \ \text{ms}^{-1}$ with an amplitude of $120 \ \text{mm}$. What is the maximum speed of a point $Q$ on the rope that is $0.4 \ \text{m}$ away from P?
Key Idea (💡): Every point on a standing or traveling string wave undergoes simple harmonic motion with a maximum vertical speed of $A\omega$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. $\frac{12}{25}\pi \text{m s}^{-1}$
Fastest Approach (🚀):
Wave frequency $f = \frac{v}{\lambda} = \frac{2.4}{1.2} = 2 \ \text{Hz}$.
Angular frequency $\omega = 2\pi f = 4\pi\text{rad/s}$.
Amplitude $A = 120\ \text{mm} = 0.12 \ \text{m}$.
Maximum transverse speed $v_{\text{max}} = A\omega = 0.12 \times 4\pi = 0.48\pi = \frac{12}{25}\pi \text{m s}^{-1}$.
Matches Option B.
Step-by-Step Breakdown:
1. Wave Equation & SHM Velocity Definitions
A. Wave Relation
$v_{\text{wave}} = f \cdot \lambda \implies f = \frac{v_{\text{wave}}}{\lambda}$
B. Angular Frequency
$\omega = 2\pi f$
C. SHM Maximum Transverse Velocity
A string particle oscillating in transverse SHM $y(t) = A \sin(\omega t + \phi)$ has maximum speed:
$v_{\text{transverse max}} = A \omega$
2. Frequency & Angular Velocity Calculation
- Wave speed $v_{\text{wave}} = 2.4 \ \text{m/s}$, Wavelength $\lambda = 1.2 \ \text{m}$.
- Frequency $f = \frac{2.4}{1.2} = 2 \ \text{Hz}$.
- Angular frequency $\omega = 2\pi(2) = 4\pi\text{rad/s}$.
3. Transverse Speed Calculation
- Amplitude $A = 120\ \text{mm} = 0.12 \ \text{m}$.
- Maximum speed of point $Q$:
$v_{\text{max}} = A \omega = 0.12 \times 4\pi = 0.48\pi \text{ m/s} = \frac{12}{25}\pi \text{m s}^{-1}$
4. Option Matching
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. $2.4 \text{ m s}^{-1}$ — Incomplete Calculation
This is the wave's propagation speed, not the transverse particle speed. - C. $\frac{3}{25}\pi \text{m s}^{-1}$ — Conceptual Misunderstanding
A factor of 1/4 error in the final calculation. - D. $\frac{6}{25}\pi \text{m s}^{-1}$ — Unit Conversion Error
A factor of 1/2 error in the calculation, caused by missing the 2 in the angular frequency formula. - E. $1.2 \text{m s}^{-1}$ — Conceptual Misunderstanding
This is the wavelength, not a speed.
Common Mistake (⚠️):
Attempting to plug the $0.4 \ \text{m}$ distance into a wave equation to find a specific instantaneous velocity instead of recognizing it asks for the maximum possible speed.
Takeaway (📌):
For any particle in a transverse wave, the maximum speed is strictly dependent on amplitude and frequency, completely independent of its position along the wave.
Question 5
Back to top ↑A capacitor of capacitance $20,000~\mu F$ is initially charged to $12 \ \text{V}$ and then allowed to discharge through a $5.6 \text{k}\Omega$ resistor. At time $t=0 \ \text{s}$, the discharge begins. What is the potential difference across the capacitor at time $t = 50 \ \text{s}$?
Key Idea (💡): Calculate time constant $\tau = RC = 5600 \times 0.02 = 112 \ \text{s}$. Exponent $-t/\tau = -50/112 \approx -0.45$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. $12 e^{-0.45}\text{ V}$
Fastest Approach (🚀):
$V_0 = 12 \ \text{V}$. Time constant $\tau = RC = 5600 \times 0.02 = 112 \ \text{s}$.
$V(50) = 12 e^{-50/112} = 12 e^{-0.45}V$.
Matches Option A.
Step-by-Step Breakdown:
1. RC Circuit Theory & Exponential Decay Laws
A. Capacitor Discharge Equation
$V(t) = V_0 e^{-t / \tau}$
B. Time Constant Definition
$\tau = R C$
2. Time Constant Calculation
- Initial voltage $V_0 = 12 \ \text{V}$.
- Resistance $R = 5.6 \text{k}\Omega = 5600\ \Omega$.
- Capacitance $C = 20,000\ \mu F = 0.02 \ \text{F}$.
- Time constant $\tau = R C = 5600 \times 0.02 = 112 \ \text{s}$.
3. Exponent Evaluation & Voltage Substitution
Discharge time $t = 50 \ \text{s}$.
Exponent ratio: $\frac{t}{\tau} = \frac{50}{112} \approx 0.45$.
$V(50) = 12 e^{-50/112} \approx 12 e^{-0.45}V$
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. $12 e^{0.45}\text{ V}$ — Unit Conversion Error
Using an exponential growth formula instead of exponential decay. - C. $6 e^{-0.45}\text{ V}$ — Conceptual Misunderstanding
Halving the initial voltage incorrectly. - D. $6 e^{0.45}\text{ V}$ — Unit Conversion Error
Halving the initial voltage and using exponential growth. - E. $24 e^{-0.45}\text{ V}$ — Conceptual Misunderstanding
Doubling the initial voltage incorrectly.
Common Mistake (⚠️):
Confusing exponential decay $e^{-x}$ with exponential growth $e^x$.
Takeaway (📌):
Capacitor discharge always follows the decay formula $V(t) = V_0 e^{-t/\tau}$.
Question 6
Back to top ↑Two parallel metal plates, P1 and P2 are separated by a distance of x. Plate P1 is maintained at voltage $V$ and P2 is earthed. A plastic sphere on the end of a string is covered in conductive paint and is suspended at the midpoint between the plates. The sphere is then given a small push towards P1. What is the subsequent behaviour of the sphere?
Key Idea (💡): Conductive objects equalize potential upon contact and experience forces in an electric field when holding a net charge.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. It swings backwards and forwards hitting each plate in turn
Fastest Approach (🚀):
Trace the charge lifecycle. Contact with plate P1 transfers positive charge, causing repulsion from P1 to P2. Contact with earthed P2 neutralises it and induces negative charge, causing attraction back to P1. It swings backwards and forwards hitting each plate in turn.
Matches Option D.
Step-by-Step Breakdown:
1. Electrostatic Conduction & Induction Principles
A. Charge Transfer by Conduction
Contact between a conductor and a voltage source $V$ forces the conductor to acquire the same electrical potential and net charge sign as the source.
B. Coulomb Repulsion & Attraction
Like charges repel ($F = q E > 0$ away from high voltage plate), opposite charges attract.
C. Earthing / Grounding
Contact with an earthed conductor ($V = 0$) neutralises net positive charge and allows negative charge to be induced under an external field.
2. Phase-by-Phase Oscillation Mechanics
- Phase 1 (Initial Contact with $P_1$): Sphere touches $P_1$ at potential $+V$, acquiring positive charge $+q$.
- Phase 2 (Repulsion toward $P_2$): Like positive charges repel $\implies$ sphere experiences force $F = +q E$ away from $P_1$ toward earthed plate $P_2$.
- Phase 3 (Contact with $P_2$): Sphere strikes earthed plate $P_2$. $+q$ drains to ground. The strong uniform field from $P_1$ induces negative charge $-q'$ on the sphere.
- Phase 4 (Attraction back to $P_1$): Negative charge $-q'$ is attracted to positive plate $P_1$, swinging it back across.
3. Sustained Electrostatic Shuttle
The process repeats continuously, shuttling charge between plates $\implies$ sphere swings backwards and forwards hitting each plate in turn.
4. Option Matching
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. It remains stationary — Unit Conversion Error
Ignoring the electrostatic forces transferred by physical contact. - B. It swings towards $P_1$ and remains in contact with the plate — Conceptual Misunderstanding
Assuming the sphere sticks due to attraction without realizing it acquires the same charge upon contact. - C. It swings back towards $P_2$ and remains in contact with the plate — Unit Conversion Error
Assuming the earthed plate permanently neutralises the sphere without inducing an opposite charge from the external field. - E. None of the above — Conceptual Misunderstanding
The sphere does indeed swing back and forth as described in D.
Common Mistake (⚠️):
Thinking the sphere will just stick to the earthed plate after losing its charge.
Takeaway (📌):
In an electric field, an earthed plate doesn't just neutralise an object. It provides charge to bring the object to $0 \ \text{V}$ locally, which in the presence of an external field leaves it with a net charge opposite to the high voltage plate.
Question 7
Back to top ↑The energy $E$ stored by a parallel plate capacitor charged to potential difference $V$ is given by $E = \frac{1}{2}QV$, where $Q = CV$ is the charge stored. Which of the following modifications results in the greatest decrease in stored energy?
Key Idea (💡): Halving $V$ reduces energy to $\left(\frac{1}{2}\right)^2 = \frac{1}{4} E_0$ (75% decrease). Halving $C$ reduces energy to $\frac{1}{2} E_0$ (50% decrease).
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. Charging the capacitor with a potential difference of $V/2$
Fastest Approach (🚀):
$E = \frac{1}{2} C V^2$.
Halving $V \implies E' = \frac{1}{4} E_0$ (75% decrease).
Halving $C \implies E' = \frac{1}{2} E_0$ (50% decrease).
Halving $V$ gives the greatest energy reduction.
Matches Option B.
Step-by-Step Breakdown:
1. Capacitor Energy Storage Laws
A. Capacitance Charge Relation
$Q = C V$
B. Energy Stored Formulas
$E = \frac{1}{2} Q V = \frac{1}{2} C V^2 = \frac{Q^2}{2C}$
2. Modification Analysis
Initial stored energy: $E_0 = \frac{1}{2} C V^2$.
- Option A ($V \to 2 \ \text{V}$): $E_A = \frac{1}{2} C (2 \ \text{V})^2 = 4 E_0$ (300% increase).
- Option B ($V \to V/2$): $E_B = \frac{1}{2} C \left(\frac{V}{2}\right)^2 = \frac{1}{4} E_0 = 0.25 E_0$ (75% decrease).
- Option C ($C \to 2C$): $E_C = \frac{1}{2} (2C) V^2 = 2 E_0$ (100% increase).
- Option D ($C \to C/2$): $E_D = \frac{1}{2} \left(\frac{C}{2}\right) V^2 = 0.5 E_0$ (50% decrease).
3. Comparison & Option Matching
Option B results in a 75% drop, which is the greatest energy reduction.
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. Charging the capacitor with a potential difference of $2V$ — Conceptual Misunderstanding
This modification increases the energy by 300%. - C. Replacing the capacitor with one of capacitance $2C$ — Conceptual Misunderstanding
This modification increases the energy by 100%. - D. Replacing the capacitor with one of capacitance $C/2$ — Conceptual Misunderstanding
This modification decreases the energy by 50%, which is less than the 75% decrease from halving V. - E. None of the above — Conceptual Misunderstanding
Option B is a valid answer as it results in a 75% reduction.
Common Mistake (⚠️):
Failing to realize that changing $V$ also changes $Q$, so $E = \frac{1}{2}CV^2$ must be used.
Takeaway (📌):
Energy stored in a capacitor depends quadratically on potential difference.
Question 8
Back to top ↑Ball A has a mass of $10 \ \text{kg}$, and ball B has a mass of X kg. They are involved in a head on collision and their directions are reversed. Prior to the collision, A had a speed of $4 \ \text{m/s}$ and B had a speed of $5 \ \text{m/s}$. After the collision, A has a speed of $2 \ \text{m/s}$ and B has a speed of $4 \ \text{m/s}$. What is the mass of B?
Key Idea (💡): In any collision free of external forces, the total momentum of the system is strictly conserved.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. $\frac{20}{3} \ \text{kg}$
Fastest Approach (🚀):
Assign direction signs (Right $+$, Left $-$):
Initial: $v_A = +4$, $v_B = -5$.
Final: $v_A' = -2$, $v_B' = +4$.
Masses: $m_A = 10$, $m_B = X$.
Conservation of momentum:
$10(4) + X(-5) = 10(-2) + X(4)$
$40 - 5X= -20 + 4X \implies 60 = 9X \implies X= 20/3 \ \text{kg}$
Matches Option D.
Step-by-Step Breakdown:
1. Conservation of Linear Momentum & Vector Direction Convention
A. Conservation Law
$p_{\text{initial total}} = p_{\text{final total}}$
B. 1D Directional Vector Mapping
Choose rightward direction as positive (+):
- Ball A initially moves right: $v_A = +4 \ \text{m/s}$.
- Ball B initially moves left: $v_B = -5 \ \text{m/s}$.
- Ball A reverses (moves left): $v_A' = -2 \ \text{m/s}$.
- Ball B reverses (moves right): $v_B' = +4 \ \text{m/s}$.
2. Momentum Balance Equation
Mass $m_A = 10 \ \text{kg}$, mass $m_B = X \ \text{kg}$.
$m_A v_A + m_B v_B = m_A v_A' + m_B v_B'$
$10(+4) + X(-5) = 10(-2) + X(+4)$
$40 - 5X= -20 + 4X$
3. Algebraic Solution for Mass $X$
$60 = 9X \implies X= \frac{60}{9} = \frac{20}{3} \ \text{kg}$
4. Option Matching
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. $5 \ \text{kg}$ — Sign Error
Making a sign error on the final velocity of A. - B. $\frac{10}{3} \ \text{kg}$ — Sign Error
Making a sign error on the initial velocity of B. - C. $\frac{15}{2} \ \text{kg}$ — Sign Error
Making a sign error on both reversed velocities. - E. $25 \ \text{kg}$ — Sign Error
Adding the momentums without respecting vector directions.
Common Mistake (⚠️):
Forgetting to make the initial velocity of B and the final velocity of A negative to account for the reversed directions.
Takeaway (📌):
Always draw a quick coordinate axis for 1D collision problems and explicitly assign positive and negative signs to velocity values before doing any algebra.
Question 9
Back to top ↑Block A and Block B are held together by a compressed spring of spring constant $k = 30 \text{N cm}^{-1}$ compressed by $20 \ \text{cm}$. When released, the spring extends and propels each block in opposite directions. The mass of block $B$ is four times that of block $A$. What are the kinetic energies of Block A and Block B after release, respectively?
Key Idea (💡): Total stored energy $E = \frac{1}{2} k x^2$. Since $p_A = p_B$, $K = \frac{p^2}{2 \text{m}}$, meaning $K_A / K_B = m_B / m_A = 4$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. $48 \ \text{J}$ and $12 \ \text{J}$
Fastest Approach (🚀):
$k = 30 \text{N cm}^{-1} = 3000 \text{N m}^{-1}$. $x = 0.2 \text{m}$.
Stored energy $E = \frac{1}{2}(3000)(0.2)^2 = 60 \ \text{J}$.
$m_B = 4 m_A \implies K_A = 4 K_B$.
$5 K_B = 60 \implies K_B = 12 \ \text{J}$ and $K_A = 48 \ \text{J}$.
Matches Option A.
Step-by-Step Breakdown:
1. Elastic Energy & Momentum-Kinetic Energy Relations
A. Hooke's Law Elastic Potential Energy
$E_{\text{elastic}} = \frac{1}{2} k x^2$
B. Kinetic Energy in Terms of Momentum
$K = \frac{p^2}{2m}$
When two bodies explode from rest, $p_A = p_B = p$, so kinetic energy is inversely proportional to mass:
$\frac{K_A}{K_B} = \frac{m_B}{m_A}$
2. Elastic Energy Calculation
- $k = 30 \text{N/cm} = 3000 \text{N/m}$.
- Compression $x = 20 \ \text{cm} = 0.20 \ \text{m}$.
- Total energy:
$E_{\text{elastic}} = \frac{1}{2} (3000) (0.20)^2 = 1500 \times 0.04 = 60 \ \text{J}$
3. Kinetic Energy Partitioning
- Mass ratio: $m_B = 4 m_A \implies K_A = 4 K_B$.
- $K_A + K_B = 60 \implies 5 K_B = 60 \implies K_B = 12 \ \text{J}$.
- $K_A = 48 \ \text{J}$.
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. $12 \ \text{J}$ and $4 \ \text{J}$ — Unit Conversion Error
Missing the 1/2 factor in the initial elastic energy calculation. - C. $8 \ \text{J}$ and $2 \ \text{J}$ — Unit Conversion Error
Making a unit conversion error with the spring constant (N/cm to N/m). - D. $48 \ \text{J}$ and $36 \ \text{J}$ — Conceptual Misunderstanding
Incorrectly assuming the energy is split proportionally to mass rather than inversely proportional. - E. $12 \ \text{J}$ and $8 \ \text{J}$ — Incomplete Calculation
An arbitrary arithmetic error during the energy partitioning.
Common Mistake (⚠️):
Assuming kinetic energy splits proportionally to mass instead of inversely proportional to mass.
Takeaway (📌):
In two-body momentum explosions, the lighter object carries the majority of kinetic energy.
Question 10
Back to top ↑Sofia is standing on an elevated platform at the same height as the back of a truck which is driving away from her at a constant speed of $20 \ \text{m/s}$. She kicks a football at an angle of $30^\circ$ to the horizontal in the direction of the truck at the same moment that the truck starts driving away. The back of the truck is $1.9 \ \text{m}$ long. If air resistance can be negated, what range of kick velocities would result in the ball landing in the back of the truck as it drives away?
Key Idea (💡): Calculate the time of flight $T$, find the ball's horizontal range $R$, and trap $R$ between the truck's minimum and maximum travel distance in time $T$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. $\frac{40}{\sqrt{3}} \le u \le \frac{40+\sqrt{1600+152\sqrt{3}}}{2\sqrt{3}}$
Fastest Approach (🚀):
Time of flight $T = \frac{2 u \sin 30^\circ}{10} = \frac{u}{10}$.
Ball range $R = u \cos 30^\circ T = \frac{\sqrt{3} u^2}{20}$.
Truck back position $x_{\text{back}} = 20 T = 2u$. Truck front $x_{\text{front}} = 2u + 1.9$.
Land inside: $2u \le \frac{\sqrt{3} u^2}{20} \le 2u + 1.9$.
Left inequality: $2u \le \frac{\sqrt{3} u^2}{20} \implies u \ge \frac{40}{\sqrt{3}}$, which matches only Option C's lower bound.
Right inequality: $\frac{\sqrt{3} u^2}{20} \le 2u + 1.9 \implies \sqrt{3}u^2 - 40u - 38 \le 0 \implies u \le \frac{40+\sqrt{1600+152\sqrt{3}}}{2\sqrt{3}} \approx 24.0 \ \text{m/s}$.
Matches Option C.
Step-by-Step Breakdown:
1. 2D Projectile Kinematics & Moving Target Constraints
A. Vertical Motion Time of Flight
$T = \frac{2 u \sin\theta}{g}$
B. Horizontal Range Formula
$R = u \cos\theta \cdot T$
C. Landing Inequality
$x_{\text{back}}(T) \le R \le x_{\text{front}}(T)$
2. Time of Flight & Ball Range Formulas
- $\theta = 30^\circ$, $g = 10 \ \text{m/s}^2$.
- Time of flight $T = \frac{2 u \sin 30^\circ}{10} = \frac{u}{10}$ seconds.
- Ball horizontal range $R = u \left(\frac{\sqrt{3}}{2}\right) \left(\frac{u}{10}\right) = \frac{\sqrt{3} u^2}{20}$ metres.
3. Moving Truck Boundaries & Inequality System
- Truck speed $v = 20$ m/s, length $L = 1.9$ m.
- Truck back at time $T$: $x_{\text{back}} = 20 T = 2u$ metres.
- Truck front at time $T$: $x_{\text{front}} = 2u + 1.9$ metres.
- Landing inequality:
$2u \le \frac{\sqrt{3} u^2}{20} \le 2u + 1.9$
4. Lower Bound Derivation & Option Matching
Solve left inequality:
$2u \le \frac{\sqrt{3} u^2}{20} \implies 40 u \le \sqrt{3} u^2 \implies u \ge \frac{40}{\sqrt{3}}$
This lower bound, $\frac{40}{\sqrt{3}}$, matches only Option C among the five choices.
5. Upper Bound Derivation & Option Matching
Solve the right inequality:
$\frac{\sqrt{3} u^2}{20} \le 2u + 1.9 \implies \sqrt{3} u^2 - 40u - 38 \le 0$
By the quadratic formula, the relevant (upper) root is:
$u \le \frac{40 + \sqrt{1600 + 152\sqrt{3}}}{2\sqrt{3}} \approx 24.0 \ \text{m/s}$
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. $\frac{20}{\sqrt{3}} \le u \le \frac{80}{\sqrt{3}} \sqrt{\frac{1600+152\sqrt{3}}{5\sqrt{3}}}$ — Unit Conversion Error
Solving both sides of the inequality unnecessarily when the lower bound alone uniquely identifies the correct answer. - B. $\frac{20}{\sqrt{3}} \le u \le \sqrt{\frac{1200+152\sqrt{3}}{2\sqrt{3}}}$ — Misapplied Formula
An arithmetic error in the quadratic formula for the upper bound. - D. $\frac{50}{\sqrt{3}} \le u \le \frac{40}{\sqrt{3}} \sqrt{\frac{1200+152\sqrt{3}}{2\sqrt{3}}}$ — Incomplete Calculation
An arithmetic error in the lower bound derivation. - E. $\frac{60}{\sqrt{3}} \le u \le \frac{40}{\sqrt{3}} \sqrt{\frac{1200+152\sqrt{3}}{2\sqrt{3}}}$ — Conceptual Misunderstanding
Miscalculating the time of flight.
Common Mistake (⚠️):
Overcomplicating the relative velocity by trying to transform the entire problem into the truck's reference frame. It's often easier to keep everything grounded in the earth frame.
Takeaway (📌):
For moving target projectile problems, solve for the time of flight first, then evaluate the position boundaries independently.
Question 11
Back to top ↑A railway carriage of mass $1000 \ \text{kg}$ is reaching the end of a track where it is stopped by a buffer which consists of an arrangement of springs. Which of the following force diagrams correctly represents the carriage, as it is stopping?
Key Idea (💡): A free body diagram must accurately reflect the direction of all forces acting on the object of interest.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. Features Normal Reaction Force, Frictional force (pointing left), Force from Spring (pointing left), Weight
Fastest Approach (🚀):
Carriage moves rightward.
Weight acts downwards, Normal reaction acts upwards.
Spring buffer pushes back to the left.
Sliding friction opposes motion and also acts to the left.
Both retarding forces point left.
Matches Option B.
Step-by-Step Breakdown:
1. Contact & Non-Contact Force Principles
A. Gravitational Force (Weight)
Acts vertically downwards through centre of mass ($W = mg$).
B. Normal Reaction Force ($N$)
Acts perpendicular to contact surface (vertically upwards).
C. Hooke's Law Spring Force
$F_s = -k x$. When compressed by rightward motion, buffer pushes back (leftwards).
D. Kinetic Friction ($f_k$)
Always opposes relative sliding velocity. For rightward motion, friction acts leftwards.
2. Directional Vector Assignment
- Carriage moves rightward ($+x$ direction).
- Vertical equilibrium: $N = mg$ ($+y$ and $-y$ forces balance).
- Horizontal forces:
- Spring force $F_s$: Points left ($-x$).
- Friction force $f_k$: Points left ($-x$).
3. Free Body Diagram Selection
Diagram B correctly shows $N$ (up), $W$ (down), $F_s$ (left), $f_k$ (left).
4. Option Matching
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. Features Normal Reaction Force, Force from Spring (pointing left), Frictional force (pointing right), Weight — Conceptual Misunderstanding
Shows the frictional force pointing right (with the direction of motion) instead of left. Friction opposes relative sliding, so it should point the same way as the spring force, not against it. - C. Features Weight (pointing up), Normal Reaction Force (pointing left), Frictional force (pointing left), Force from Spring (pointing down) — Sign Error
Identifying the correct forces, but showing the spring force pointing in the wrong direction (down instead of left). - D. Features Force from Spring (pointing up), Frictional force (pointing left), Normal Reaction Force (pointing left), Weight (pointing down) — Conceptual Misunderstanding
Showing the spring force pointing up instead of left. - E. Features Normal Reaction Force, Frictional force, Weight, Force from Spring — Sign Error
Listing the correct forces but failing to specify their directional vectors.
Common Mistake (⚠️):
Assuming friction always acts in the opposite direction of the main applied force. Friction opposes relative motion, not other forces.
Takeaway (📌):
When an object is braking or decelerating, all contact retarding forces point backward.
Question 12
Back to top ↑Alex and Ben investigate fluid flow in a pipe. They relate shear stress $\tau$ to dynamic viscosity $\mu$ and velocity gradient $\frac{dv}{dy}$. Which of the following equations is dimensionally consistent?
Key Idea (💡): Newton's law of viscosity states $\tau = -\mu \frac{dv}{dy}$ where shear stress $\tau$ has units of $Pa$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. $\tau = -\mu \frac{dv}{dy}$ with $[\tau] = Pa$
Fastest Approach (🚀):
Stress is Force / Area $\implies Pa$. Formula is linear in $\mu$ and $\frac{dv}{dy}$.
Matches Option A.
Step-by-Step Breakdown:
1. Fluid Shear Stress & Viscosity Definitions
A. Shear Stress ($\tau$)
Tangential force per unit area parallel to fluid layers:
$[\tau] = \frac{\text{Force}}{\text{Area}} = \frac{N}{m^2} = Pa$
B. Newton's Law of Viscosity
In laminar fluid flow, shear stress is directly proportional to the velocity gradient:
$\tau = -\mu \frac{dv}{dy}$
2. Dimensional Verification
- $[\frac{dv}{dy}] = \frac{\text{m s}^{-1}}{m} = s^{-1}$.
- Dynamic viscosity $[\mu] = \text{Pa s} = \text{N s m}^{-2}$.
- Right Hand Side dimensions: $[\mu \frac{dv}{dy}] = (\text{Pa s}) \times (s^{-1}) = Pa$.
- Dimensions match Left Hand Side $[\tau] = Pa$.
3. Distractor Elimination
- Option B uses $\text{N m}^{-1}$ (surface tension, not stress).
- Options C & D use incorrect non-linear powers of viscosity $\mu^2$ or $\mu^{-1}$.
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. $\tau = -\mu \frac{dv}{dy}$ with $[\tau] = \text{N m}^{-1}$ — Unit Conversion Error
Using the units for surface tension (N m^-1) instead of shear stress (N m^-2). - C. $\tau = -\mu^2 \frac{dv}{dy}$ with $[\tau] = Pa$ — Unit Conversion Error
Using an incorrect non-linear power of viscosity (mu^2). - D. $\tau = -\mu^{-1} \frac{dv}{dy}$ with $[\tau] = \text{N m}^{-1}$ — Unit Conversion Error
Using an incorrect inverse power of viscosity. - E. $\tau = -\mu^2 \frac{dv}{dy}$ with $[\tau] = \text{N m}^{-1}$ — Unit Conversion Error
Using both the wrong units and the wrong power of viscosity.
Common Mistake (⚠️):
Confusing shear stress units ($\text{N m}^{-2}$) with surface tension units ($\text{N m}^{-1}$).
Takeaway (📌):
Stress of any kind is defined as Force per unit Area (Pascals).
Question 13
Back to top ↑Two cars, A and B, are $60 \ \text{m}$ apart at time $t=0$. Car A accelerates from rest towards Car B with a constant acceleration of $6.0 \text{m s}^{-2}$. Car B moves away from Car A with an initial velocity of $2.0 \text{m s}^{-1}$ and an acceleration of $4.0 \text{m s}^{-2}$. How far from Car B's starting point do the two cars meet?
Key Idea (💡): Equate position functions $x_A(t) = x_B(t)$ from a common origin to find collision time.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. $170 \ \text{m}$
Fastest Approach (🚀):
$3t^2 = 60 + 2t + 2t^2 \implies t^2 - 2t - 60 = 0 \implies t = 1 + \sqrt{61} \approx 8.81 \ \text{s}$.
Distance from B's start $= 2(8.81) + 2(8.81)^2 \approx 173 \ \text{m} \approx 170 \ \text{m}$.
Matches Option C.
Step-by-Step Breakdown:
1. SUVAT Kinematics & Relative Displacement Equations
A. Position Formula
$x(t) = x_0 + v_0 t + \frac{1}{2} a t^2$
B. Intersection Condition
$x_A(t) = x_B(t)$
2. Position Equations Formulation
- Origin at Car A's starting point ($x_{0A} = 0$).
- Car A: $v_{0A} = 0, a_A = 6.0 \ \text{m/s}^2 \implies x_A(t) = 3t^2$.
- Car B: $x_{0B} = 60 \ \text{m}, v_{0B} = 2.0 \ \text{m/s}, a_B = 4.0 \ \text{m/s}^2 \implies x_B(t) = 60 + 2t + 2t^2$.
3. Collision Time & Car B Displacement
Set $x_A(t) = x_B(t)$:
$3t^2 = 60 + 2t + 2t^2 \implies t^2 - 2t - 60 = 0$
Solve quadratic:
$t = \frac{2 + \sqrt{4 - 4(-60)}}{2} = 1 + \sqrt{61} \approx 8.81 \ \text{s}$
Distance moved by Car B from ITS starting position:
$\Delta x_B = v_{0B} t + \frac{1}{2} a_B t^2 = 2(8.81) + 2(8.81)^2 \approx 172.85 \ \text{m} \approx 170 \ \text{m}$
4. Option Matching
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. $460 \ \text{m}$ — Conceptual Misunderstanding
Calculating the distance from Car A's origin instead of Car B's starting point, and making a calculation error. - B. $230 \ \text{m}$ — Conceptual Misunderstanding
Calculating the total distance from Car A's origin, not Car B's starting point. - D. $1.7 \ \text{s}$ — Sign Error
Making a sign error when solving the quadratic equation. - E. $8.8 \ \text{s}$ — Unit Conversion Error
This is the time to collision in seconds, not the distance.
Common Mistake (⚠️):
Calculating total distance from A's origin ($232.8 \ \text{m}$) instead of distance from B's starting point.
Takeaway (📌):
Pay close attention to the origin reference point when computing relative displacements.
Question 14
Back to top ↑Two plane waves of equal frequency pass through two parallel slits separated by a distance $x$, travelling at an angle $\theta$ to the normal of the slits. What is the phase difference between the waves as they pass through the slits?
Key Idea (💡): Phase difference $\Delta \phi$ is fundamentally related to physical path difference $\Delta L$ by the ratio of full circles to wavelength: $\Delta \phi = \frac{2\pi}{\lambda} \Delta L$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. $2\pi x \sin(\theta)/\lambda$
Fastest Approach (🚀):
Path difference $\Delta L = x \sin\theta$.
Multiply by wave number $k = \frac{2\pi}{\lambda}$:
$\text{Phase Difference} = \frac{2\pi x \sin\theta}{\lambda}$
Matches Option A.
Step-by-Step Breakdown:
1. Geometric Path Difference ($\Delta L$)
When two parallel waves pass through slits separated by a distance $x$ at an angle $\theta$ to the normal, one wave must travel slightly further than the other to reach a distant screen.
If we drop a perpendicular line from the top slit to the path of the bottom wave, we form a small right-angled triangle.
The hypotenuse of this triangle is the slit separation, $x$.
The opposite side of this triangle represents the extra distance travelled by the lower wave, known as the path difference $\Delta L$.
Using basic trigonometry (SOH CAH TOA):
$\sin\theta = \frac{\text{Opposite}}{\text{Hypotenuse}} = \frac{\Delta L}{x}$
Rearranging for $\Delta L$:
$\Delta L = x \sin\theta$
2. Converting Path to Phase Difference ($\Delta \phi$)
A full wavelength $\lambda$ corresponds to a full phase cycle of $2\pi$ radians.
Therefore, to convert any physical path difference into a phase angle, we multiply the path difference by the fraction of a full cycle it represents per metre (the wave number, $k = \frac{2\pi}{\lambda}$).
$\Delta \phi = \frac{2\pi}{\lambda} \cdot \Delta L$
3. Final Derivation
Substitute the geometric path difference $\Delta L = x \sin\theta$ into the phase equation:
$\Delta \phi = \frac{2\pi}{\lambda} (x \sin\theta) = \frac{2\pi x \sin\theta}{\lambda}$
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. $\pi x \sin(\theta)/\lambda$ — Unit Conversion Error
Using pi instead of 2*pi to represent a full phase cycle. - C. $\pi x \sin(\theta)/2\lambda$ — Conceptual Misunderstanding
Introducing a mistaken factor of 2 in the denominator. - D. $2x \sin(\theta)/\pi\lambda$ — Unit Conversion Error
Inverting the ratio, placing pi and lambda incorrectly. - E. $x \sin(\theta)/\lambda$ — Conceptual Misunderstanding
Forgetting the 2*pi factor entirely when converting from wavelengths to radians.
Common Mistake (⚠️):
Using just $\pi$ instead of $2\pi$ for a full phase cycle, or confusing the path difference formula with diffraction grating formulas.
Takeaway (📌):
To convert a physical path difference in metres to a phase difference in radians, simply multiply by $2\pi / \lambda$.
Question 15
Back to top ↑$ {}^{235}_{92}U$ decays to $ {}^{207}_{82}Pb$. What are the decay products?
Key Idea (💡): Alpha decays strictly handle mass reduction. Beta decays adjust the final proton count once the mass is balanced.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. $7\alpha+4\beta^-$
Fastest Approach (🚀):
Mass change: $235 - 207 = 28$. Alpha count $= 28 / 4 = 7$.
Seven alphas reduce atomic number by $7 \times 2 = 14 \implies 92 - 14 = 78$.
Final atomic number is $82 \implies 82 - 78 = 4\ \beta^-$ particles.
Total: $7\alpha + 4\beta^-$.
Matches Option B.
Step-by-Step Breakdown:
1. Conservation Laws in Radioactive Decay
A. Mass Number Conservation
$\sum A_{\text{reactants}} = \sum A_{\text{products}}$
B. Atomic Number Conservation
$\sum Z_{\text{reactants}} = \sum Z_{\text{products}}$
C. Decay Particle Signatures
- Alpha particle: $\alpha = {}^4_2 \text{He}$ ($A=4, Z=2$).
- Beta minus particle: $\beta^- = {}^{\ 0}_{-1}\text{e}$ ($A=0, Z=-1$).
2. Balancing Mass Numbers ($A$) for Alpha Count
Change in mass: $\Delta A = 235 - 207 = 28$.
Since $\beta^-$ has zero mass number:
$N_\alpha = \frac{\Delta A}{4} = \frac{28}{4} = 7\ \alpha \text{particles}$
3. Balancing Atomic Numbers ($Z$) for Beta Count
- Initial $Z_i = 92$.
- Reduction from 7 alpha decays: $7 \times 2 = 14 \implies Z_{\text{intermediate}} = 92 - 14 = 78$.
- Target $Z_f = 82$.
- Deficit in atomic number: $\Delta Z = 82 - 78 = +4$.
- Since each $\beta^-$ increases $Z$ by $+1$:
$N_\beta = 4\ \beta^-\text{particles}$
Total products: $7\alpha + 4\beta^-$.
4. Option Matching
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. $8\alpha+6\beta^-$ — Conceptual Misunderstanding
Miscalculating the initial mass difference. - C. $6\alpha+4\beta^-$ — Unit Conversion Error
A simple arithmetic error when subtracting the alpha particles' mass. - D. $5\alpha+3\beta^-$ — Conceptual Misunderstanding
Miscalculating both the mass difference and the required atomic number adjustment. - E. $4\alpha+2\beta^-$ — Unit Conversion Error
Misinterpreting the beta decay effect on the atomic number.
Common Mistake (⚠️):
Confusing Beta minus decay with Beta plus decay, causing the atomic number to be subtracted instead of added.
Takeaway (📌):
Always balance mass numbers first using alpha particles, as beta particles have a mass number of zero.
Question 16
Back to top ↑In a laboratory experiment, protactinium-234 undergoes radioactive decay by $\beta^-$ emission into uranium-234. The table below describes how the mass of uranium-234 present in the sample varies with time from the start of the experiment. Using the information in the table, approximately what is the half-life of protactinium-234?
Key Idea (💡): The half-life of a radioactive isotope is the time taken for half of the initial nuclei in a sample to decay.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. 1.2 minutes
Fastest Approach (🚀):
As $t \to \infty$, the mass of U-234 reaches $16.0 \ \text{mg} \implies$ initial Pa-234 mass was $16.0 \ \text{mg}$.
Half-life occurs when half has decayed $\implies M_U = 8.0 \ \text{mg}$.
From table, $M_U = 8.0 \ \text{mg}$ at $t = 1.2\ \text{minutes}$.
Matches Option A.
Step-by-Step Breakdown:
1. Parent-Daughter Decay Kinematics
A. Mass Conservation Law
$M_{\text{parent}}(t) + M_{\text{daughter}}(t) = M_0$
B. Half-Life Definition
The time $t_{1/2}$ at which $M_{\text{parent}}(t_{1/2}) = \frac{1}{2} M_0 \implies M_{\text{daughter}}(t_{1/2}) = \frac{1}{2} M_0$.
2. Initial Mass Determination
- Decay process: $^{234}Pa \to {}^{234}\text{U} + \beta^-$.
- As $t \to \infty$, all parent nuclei have decayed, so $M_{\text{daughter}}(\infty) = M_0 = 16.0 \ \text{mg}$.
3. Half-Life Lookup
- Half-life target: $M_{\text{daughter}}(t_{1/2}) = \frac{16.0}{2} = 8.0 \ \text{mg}$.
- From the experiment data table, $M_{\text{daughter}} = 8.0 \ \text{mg}$ at $t = 1.2\ \text{minutes}$.
- Half-life $t_{1/2} = 1.2\ \text{minutes}$.
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. 2.4 minutes — Unit Conversion Error
Misinterpreting the asymptote and taking half of an incorrect maximum value. - C. 6.0 minutes — Conceptual Misunderstanding
Reading the time for 15.5 mg instead of the halfway point. - D. 9.6 minutes — Unit Conversion Error
Misinterpreting the table data completely. - E. 10.8 minutes — Unit Conversion Error
Misinterpreting the table data. - F. 12.0 minutes — Conceptual Misunderstanding
Taking the final time recorded in the table as the half-life.
Common Mistake (⚠️):
Misinterpreting the table as the mass of the parent isotope remaining, which would lead to incorrect half-life calculations.
Takeaway (📌):
For a parent-daughter isotope pair, the sum of their masses (or number of nuclei) remains constant. Identify the asymptote to find the initial sample mass.
Question 17
Back to top ↑The depth of water in a tidal harbour oscillates periodically between a minimum depth of $10 \ \text{m}$ and a maximum depth of $16 \ \text{m}$ with a period of $12\ \text{hours}$. Treating this tidal variation as a wave, what are the amplitude and frequency of this wave?
Key Idea (💡): Amplitude is half the peak-to-peak displacement. Frequency is $f = 1 / T$ with period $T$ in seconds.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. Amplitude: $3 \ \text{m}$, Frequency: $\frac{1}{12 \times 3600}Hz$
Fastest Approach (🚀):
Amplitude $= \frac{16 - 10}{2} = 3 \ \text{m}$.
Period $T = 12 \times 3600 \ \text{s} \implies f = \frac{1}{12 \times 3600}Hz$.
Matches Option A.
Step-by-Step Breakdown:
1. Oscillatory Wave Parameter Laws
A. Equilibrium Midpoint
$y_0 = \frac{y_{\text{max}} + y_{\text{min}}}{2}$
B. Amplitude Formula
$A = y_{\text{max}} - y_0 = \frac{y_{\text{max}} - y_{\text{min}}}{2}$
C. Frequency Period Relation
$f = \frac{1}{T} \quad (T \text{in seconds})$
2. Amplitude Calculation
- $y_{\text{max}} = 16 \ \text{m}, y_{\text{min}} = 10 \ \text{m}$.
- $A = \frac{16 - 10}{2} = 3 \ \text{m}$.
3. Frequency Calculation
- Period $T = 12\ \text{hours} = 12 \times 3600\ \text{seconds}$.
- Frequency:
$f = \frac{1}{12 \times 3600}Hz$
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. Amplitude: $3 \ \text{m}$, Frequency: $\frac{3600}{12}Hz$ — Unit Conversion Error
Inverting the frequency formula incorrectly. - C. Amplitude: $6 \ \text{m}$, Frequency: $\frac{1}{24 \times 3600}Hz$ — Unit Conversion Error
Confusing amplitude with the total peak-to-peak depth variation (6 m). - D. Amplitude: $6 \ \text{m}$, Frequency: $\frac{3600}{24}Hz$ — Unit Conversion Error
Using the wrong amplitude and inverting the frequency formula. - E. Amplitude: $8 \ \text{m}$, Frequency: $\frac{1}{12 \times 3600}Hz$ — Unit Conversion Error
Using the maximum depth instead of the amplitude. - F. Amplitude: $8 \ \text{m}$, Frequency: $\frac{3600}{12}Hz$ — Unit Conversion Error
Using the maximum depth and inverting the frequency. - G. Amplitude: $16 \ \text{m}$, Frequency: $\frac{1}{24 \times 3600}Hz$ — Unit Conversion Error
Using the peak depth and assuming a 24 hour period. - H. Amplitude: $16 \ \text{m}$, Frequency: $\frac{3600}{24}Hz$ — Unit Conversion Error
Using the peak depth and inverting a 24 hour period.
Common Mistake (⚠️):
Confusing amplitude with peak-to-peak depth variation ($6 \ \text{m}$).
Takeaway (📌):
Amplitude is half the total range from minimum to maximum.
Question 18
Back to top ↑When radioactive isotopes decay, they sometimes have to go through a succession of disintegrations to reach a stable isotope. These are called decay chains and involve the successive emission of numerous $\alpha$ and/or $\beta$ particles. One such isotope is radon-219, which goes through a chain in which three $\alpha$ particles and two $\beta^-$ particles are emitted before reaching a stable isotope. What are the atomic and mass numbers of the resulting isotope?
Key Idea (💡): An alpha decay decreases the mass number by 4 and atomic number by 2. A beta-minus decay does not change the mass number and increases the atomic number by 1.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. Atomic number 82, Mass number 207
Fastest Approach (🚀):
Mass number: $219 - 3(4) = 207$.
Atomic number: $86 - 3(2) + 2(1) = 82$.
Matches Option C.
Step-by-Step Breakdown:
1. Nuclear Decay Transformation Rules
A. Alpha Decay ($\alpha = {}^4_2 \text{He}$)
$\Delta A = -4, \quad \Delta Z = -2$
B. Beta-Minus Decay ($\beta^- = {}^{\ 0}_{-1}\text{e}$)
$\Delta A = 0, \quad \Delta Z = +1$
2. Initial Isotope Coordinates
- Starting isotope: Radon-219 ($_{86}^{219}\text{Rn}$).
- Initial mass number $A_i = 219$.
- Initial atomic number $Z_i = 86$.
3. Decay Chain Arithmetic
- Decay process: $3\alpha + 2\beta^-$.
- Mass number calculation:
- Atomic number calculation:
$A_f = 219 - 3(4) - 2(0) = 219 - 12 = 207$
$Z_f = 86 - 3(2) + 2(1) = 86 - 6 + 2 = 82$
4. Option Matching
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. Atomic number 80, Mass number 207 — Sign Error
Forgetting that beta-minus emission increases the atomic number, rather than decreasing it. - B. Atomic number 80, Mass number 211 — Incomplete Calculation
Miscalculating the mass number change from the alpha particles. - D. Atomic number 82, Mass number 215 — Unit Conversion Error
Calculating the mass change for only a single alpha particle decay. - E. Atomic number 85, Mass number 211 — Sign Error
Making a sign error when adjusting the atomic number. - F. Atomic number 85, Mass number 219 — Conceptual Misunderstanding
Assuming no mass change occurred during the decays. - G. Atomic number 86, Mass number 215 — Sign Error
Making a sign error when adjusting the atomic number. - H. Atomic number 86, Mass number 219 — Conceptual Misunderstanding
Forgetting to change the atomic and mass numbers altogether.
Common Mistake (⚠️):
Forgetting that beta-minus emission increases the atomic number by $1$, leading to an incorrect atomic number of $80$ (Option A).
Takeaway (📌):
Keep track of charge and mass conservation. Alpha: $\Delta A = -4, \Delta Z = -2$. Beta-minus: $\Delta A = 0, \Delta Z = +1$.
Question 19
Back to top ↑The circuit shows five identical filament bulbs designed to work at $12 \ \text{V}$ connected in a circuit with two switches. Switch P is initially open and switch Q is initially closed. Switch P is then closed and switch Q is opened. Compared with the brightness before these changes were made, how has the brightness of Bulbs X and Y changed?
Key Idea (💡): Bulb brightness is determined by the electrical power it dissipates ($P = I^2 R$). Total current in a series-parallel network changes when the equivalent resistance is altered by switches.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. Bulb X: Brighter, Bulb Y: Dimmer
Fastest Approach (🚀):
Initial state (P open, Q closed): $R_{\text{total}} = 2.5R \implies I_y= 0.4 \ \text{V/R}, I_x= 0.2 \ \text{V/R}$.
Final state (P closed, Q open): Bottom branch open-circuited $\implies R_{\text{total}} = 3R \implies I_y= I_x= 0.33 \ \text{V/R}$.
Bulb X: $0.2 \to 0.33 \implies$ Brighter.
Bulb Y: $0.4 \to 0.33 \implies$ Dimmer.
Matches Option B.
Step-by-Step Breakdown:
1. DC Circuit Laws & Filament Bulb Brightness
A. Bulb Brightness Law
Dissipated power $P = I^2 R$. Brightness depends directly on current magnitude $I$.
B. Series & Parallel Equivalent Resistance
$R_{\text{series}} = R_1 + R_2, \quad R_{\text{parallel}} = \frac{R_1 R_2}{R_1 + R_2}$
2. Initial Circuit Analysis (P Open, Q Closed)
- Parallel sub-network 1 (Bulb X || bottom-left): $R_{p1} = 0.5R$.
- Sub-network 2 (bottom-middle): $R_{p2} = R$.
- Series combination of the two sub-networks: $R_p = 0.5R + R = 1.5R$.
- Total circuit resistance: $R_{\text{initial}} = 1.5R + R = 2.5R$.
- Total current (through Bulb Y): $I_{Y, \text{initial}} = \frac{V}{2.5R} = 0.4 \frac{V}{R}$.
- Voltage drop across $R_{p1} = 0.4 \frac{V}{R} \times 0.5R = 0.2 \ \text{V}$.
- Current through Bulb X: $I_{X, \text{initial}} = \frac{0.2 \ \text{V}}{R} = 0.2 \frac{V}{R}$.
3. Final Circuit Analysis (P Closed, Q Open)
- Q open $\implies$ bottom wire open-circuited (disabling both bottom bulbs).
- P closed $\implies$ top row (Bulb X + top-middle bulb) forms series branch of $2R$.
- Total circuit resistance: $R_{\text{final}} = 2R + R = 3R$.
- Total current (through BOTH X and Y): $I_{X, \text{final}} = I_{Y, \text{final}} = \frac{V}{3R} \approx 0.333 \frac{V}{R}$.
4. Brightness Comparison & Option Matching
- Bulb X: $0.20 \frac{V}{R} \to 0.333 \frac{V}{R} \implies$ Brighter.
- Bulb Y: $0.40 \frac{V}{R} \to 0.333 \frac{V}{R} \implies$ Dimmer.
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. Bulb X: Brighter, Bulb Y: Brighter — Conceptual Misunderstanding
Incorrectly determining the final current distribution. - C. Bulb X: Dimmer, Bulb Y: Brighter — Unit Conversion Error
Miscalculating the equivalent resistance and assuming Bulb X gets less current. - D. Bulb X: Dimmer, Bulb Y: Dimmer — Conceptual Misunderstanding
Incorrectly assuming both bulbs receive less current due to the open switch. - E. Bulb X: Unchanged, Bulb Y: Brighter — Conceptual Misunderstanding
Assuming the series Bulb X doesn't change because the battery voltage is constant. - F. Bulb X: Brighter, Bulb Y: Unchanged — Conceptual Misunderstanding
Assuming Bulb Y's brightness doesn't change.
Common Mistake (⚠️):
Assuming the total current is constant, or failing to realize that opening Switch Q open-circuits the entire bottom branch.
Takeaway (📌):
Calculate equivalent resistances for both states to determine current changes through specific components.
Question 20
Back to top ↑In an ornamental fountain, water is squirted vertically through the nozzle by a pump. $5 \ \text{kg}$ of water pass through the nozzle each second, and the water reaches a height of $5 \ \text{m}$ after leaving the nozzle. What is the power of the pump (assuming 100% efficiency), and at what speed does the water leave the nozzle? Take g to be $10 \ \text{N/kg}$.
Key Idea (💡): By conservation of energy, the kinetic energy of water leaving the nozzle equals its potential energy at peak height. Power is energy per unit time.
Reveal the answer & worked solution — commit to an option first
Correct Answer: G. Power: $250 \ \text{W}$, Speed: $10 \ \text{m/s}$
Fastest Approach (🚀):
Speed: $v = \sqrt{2gh} = \sqrt{2 \times 10 \times 5} = 10 \ \text{m/s}$.
Power: $P = \frac{1}{2} \left(\frac{dm}{dt}\right) v^2 = 0.5 \times 5 \times 100 = 250 \ \text{W}$.
Matches Option G.
Step-by-Step Breakdown:
1. Conservation of Energy & Fluid Kinetic Power Principles
A. Torricelli Energy Conservation
$\frac{1}{2} m v^2 = m g h \implies v = \sqrt{2gh}$
B. Mass Flow Kinetic Power Formula
$P = \frac{d E_k}{dt} = \frac{1}{2} \left(\frac{dm}{dt}\right) v^2$
2. Leaving Speed Calculation
- Maximum height $h = 5 \ \text{m}, g = 10 \text{N/kg}$.
- Exit speed: $v = \sqrt{2 \times 10 \times 5} = 10 \ \text{m/s}$.
3. Pump Power Calculation
- Mass flow rate $\dot{m} = 5\ \text{kg/s}$.
- Pump power output:
$P = \frac{1}{2} \times (5\ \text{kg/s}) \times (10 \ \text{m/s})^2 = 2.5 \times 100 = 250 \ \text{W}$
4. Option Matching
Matches Option G.
Why the Other Options Are Wrong (❌):
- A. Power: $5 \ \text{W}$, Speed: $5 \ \text{m/s}$ — Misapplied Formula
Miscalculating both the exit speed and power. - B. Power: $5 \ \text{W}$, Speed: $50 \ \text{m/s}$ — Incomplete Calculation
Making an arithmetic error in the speed calculation. - C. Power: $25 \ \text{W}$, Speed: $10 \ \text{m/s}$ — Misapplied Formula
Calculating the correct speed but making a factor of 10 error on power. - D. Power: $25 \ \text{W}$, Speed: $100 \ \text{m/s}$ — Unit Conversion Error
Using the wrong power formula. - E. Power: $50 \ \text{W}$, Speed: $5 \ \text{m/s}$ — Unit Conversion Error
Using the wrong power formula. - F. Power: $50 \ \text{W}$, Speed: $50 \ \text{m/s}$ — Unit Conversion Error
Using the wrong power formula. - H. Power: $250 \ \text{W}$, Speed: $100 \ \text{m/s}$ — Conceptual Misunderstanding
Making a factor of 10 error on the speed calculation.
Common Mistake (⚠️):
Calculating power as $mgh = 5 \times 10 \times 5 = 250$ W but getting the speed formula wrong, or using $P = mgh$ directly without confirming the kinetic energy transfer rate.
Takeaway (📌):
Use conservation of energy to link velocity and height ($v = \sqrt{2gh}$), and power to the rate of kinetic energy delivery ($P = \frac{1}{2} \dot{m} v^2$).
Question 21
Back to top ↑A car of mass $800 \ \text{kg}$ moves up an incline of 1 in 20 (1 in 20 means for every $20 \ \text{m}$ along the road the car gains $1 \ \text{m}$ in height) at a constant speed of $20 \ \text{m/s}$. The frictional force opposing motion is $500 \ \text{N}$. Taking $g$ to be $10 \ \text{N/kg}$, how much work has been done by the engine after the car has moved $50 \ \text{m}$?
Key Idea (💡): At constant speed, the engine must exert a force equal to the sum of the gravitational component down the slope and the frictional force.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. 45 kJ
Fastest Approach (🚀):
Parallel gravity force: $mg \sin(\theta) = 800 \times 10 \times \frac{1}{20} = 400 \ \text{N}$.
Frictional force: $500 \ \text{N}$.
Total engine force: $400 + 500 = 900 \ \text{N}$.
Work done: $W = F \times d = 900 \times 50 = 45,000 \text{J} = 45 \text{kJ}$.
Matches Option D.
Step-by-Step Breakdown:
1. Incline Geometry & Newton's First Law Principles
A. Incline Ratio Rule
Slope ratio $1\ \text{in }20 \implies \sin\theta = \frac{1}{20}$.
B. Gravitational Slope Force
$F_{g\parallel} = mg \sin\theta$
C. Constant Speed Equilibrium
$\sum F = 0 \implies F_{\text{engine}} = F_{g\parallel} + f_{\text{friction}}$
2. Opposing Force Summation
- Mass $m = 800 \ \text{kg}, g = 10 \text{N/kg}, \sin\theta = \frac{1}{20}$.
- Parallel gravity force: $F_{g\parallel} = 800 \times 10 \times \frac{1}{20} = 400 \ \text{N}$.
- Friction: $f = 500 \ \text{N}$.
- Engine force required: $F_{\text{engine}} = 400 + 500 = 900 \ \text{N}$.
3. Work Calculation
Distance $d = 50 \ \text{m}$.
$W = F_{\text{engine}} \times d = 900 \times 50 = 45,000\ \text{J} = 45 \text{kJ}$
4. Option Matching
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. 20 kJ — Unit Conversion Error
Forgetting to include the frictional force opposing motion. - B. 25 kJ — Unit Conversion Error
Forgetting to include the gravitational force opposing motion. - C. 27 kJ — Incomplete Calculation
Making an arithmetic error when summing the forces. - E. 65 kJ — Conceptual Misunderstanding
Miscalculating the gravitational component. - F. 160 kJ — Unit Conversion Error
Using cosine instead of sine for the slope.
Common Mistake (⚠️):
Forgetting the frictional force ($500$ N), which would give $W = 400 \times 50 = 20$ kJ (Option A).
Takeaway (📌):
Ensure all opposing forces (both gravity component and friction) are summed when calculating the required engine force for constant-speed motion.
Question 22
Back to top ↑A bullet of mass $50 \ \text{g}$ is fired from a rifle with a velocity of $300 \ \text{m/s}$. It hits the bank of earth and after travelling $60 \ \text{cm}$ into the bank comes to rest. What is the average stopping force of the earth in the bank on the bullet?
Key Idea (💡): The work done by the average stopping force equals the initial kinetic energy of the bullet.
Reveal the answer & worked solution — commit to an option first
Correct Answer: B. $3.75 \times 10^3 \ \text{N}$
Fastest Approach (🚀):
Initial kinetic energy: $E_k = 0.5 \times 0.05 \times 300^2 = 2250 \ \text{J}$.
Stopping force: $F = \frac{E_k}{s} = \frac{2250}{0.6} = 3750 \text{N} = 3.75 \times 10^3 \ \text{N}$.
Matches Option B.
Step-by-Step Breakdown:
1. Work-Energy Theorem & SI Unit Laws
A. Kinetic Energy Formula
$K = \frac{1}{2} m u^2$
B. Work-Energy Theorem
$W_{\text{net}} = \Delta K \implies F \cdot s = \frac{1}{2} m u^2$
2. Initial Kinetic Energy Calculation
- $m = 50\ \text{g} = 0.05 \ \text{kg}, u = 300 \ \text{m/s}$.
- $K = \frac{1}{2} (0.05) (300)^2 = 0.025 \times 90,000 = 2250 \ \text{J}$.
3. Average Stopping Force Calculation
- Penetration distance $s = 60 \ \text{cm} = 0.60 \ \text{m}$.
- $F \times 0.60 = 2250 \implies F = \frac{2250}{0.60} = 3750 \text{N} = 3.75 \times 10^3 \ \text{N}$.
4. Option Matching
Matches Option B.
Why the Other Options Are Wrong (❌):
- A. $37.5 \ \text{N}$ — Conceptual Misunderstanding
Failing to convert grams to kilograms, resulting in an error of 1000. - C. $3.75 \times 10^4 \ \text{N}$ — Conceptual Misunderstanding
Making an order of magnitude error with the decimal point. - D. $3.75 \times 10^6 \ \text{N}$ — Conceptual Misunderstanding
Failing to convert the stopping distance from cm to m. - E. $3.75 \times 10^5 \ \text{N}$ — Incomplete Calculation
Squaring the mass or making another arithmetic error.
Common Mistake (⚠️):
Failing to convert units (like using mass in grams or distance in centimetres), which leads to an error of several orders of magnitude.
Takeaway (📌):
Always perform calculations in SI base units (kg, m, s) to ensure scientific notation prefixes are correct.
Question 23
Back to top ↑A circuit consists of a battery connected in series with a resistor of resistance $3R$ and a resistor of resistance $2R$. A voltmeter connected across the $3R$ resistor measures a potential difference of $V$. What is the total potential difference across the battery?
Key Idea (💡): For series resistors, voltage is divided proportional to resistance: $\frac{V_1}{V_{\text{total}}} = \frac{R_1}{R_{\text{total}}}$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. $\frac{5}{3}V$
Fastest Approach (🚀):
$V_{\text{battery}} = V \times \frac{3R + 2R}{3R} = \frac{5}{3}V$.
Matches Option C.
Step-by-Step Breakdown:
1. Potential Divider Theorem & Series Resistors
A. Series Current Law
Same current $I$ flows through all components in series.
B. Potential Divider Relation
$\frac{V_1}{V_{\text{total}}} = \frac{R_1}{R_{\text{total}}}$
2. Resistance & Current Formulation
- Measured resistor $R_1 = 3R$, second resistor $R_2 = 2R$.
- Total series resistance: $R_{\text{total}} = 3R + 2R = 5R$.
- Circuit current: $I = \frac{V}{3R}$.
3. Total Battery Voltage Calculation
$V_{\text{battery}} = I \cdot R_{\text{total}} = \left(\frac{V}{3R}\right) \cdot (5R) = \frac{5}{3} V$
4. Option Matching
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. $\frac{8}{3}V$ — Misapplied Formula
Setting up the ratio incorrectly. - B. $5 \ \text{V}$ — Incomplete Calculation
Dropping the fractional part. - D. $\frac{3}{5}V$ — Unit Conversion Error
Setting up the potential divider ratio to find the voltage across the 3R resistor, rather than solving for the battery voltage. - E. $2 \ \text{V}$ — Incomplete Calculation
An arithmetic error in the fraction.
Common Mistake (⚠️):
Calculating $\frac{3}{5}V$ (Option D) instead of solving for battery voltage.
Takeaway (📌):
In series circuits, battery voltage is $V_{\text{total}} = V_{\text{measured}} \times \frac{R_{\text{total}}}{R_{\text{measured}}}$.
Question 24
Back to top ↑Sound wave A and sound wave B propagate in the same uniform medium. Wave A has the same amplitude as Wave B, but half the wavelength of Wave B. Consider the following statements:
I. The intensity of Wave A is greater than the intensity of Wave B.
II. Wave A is heard at a higher pitch than Wave B.
III. The propagation speed of Wave A is greater than the propagation speed of Wave B.
Which of these statements is/are correct?
Key Idea (💡): Wave speed is determined solely by the medium. Pitch is determined by frequency ($f = v / \lambda$). Intensity depends on BOTH amplitude and frequency ($I \propto A^2 f^2$), not amplitude alone.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. I and II
Fastest Approach (🚀):
Speed depends on medium $\implies$ equal speeds (III false).
$\lambda_A = \frac{1}{2} \lambda_B \implies f_A = 2 f_B \implies$ higher pitch (II true).
Intensity $I \propto A^2 f^2$. Same amplitude, but $f_A = 2f_B \implies I_A = A^2(2f_B)^2 = 4 A^2 f_B^2 = 4 I_B$, so Wave A's intensity IS greater (I true).
Matches Option D (I and II).
Step-by-Step Breakdown:
1. Wave Propagation Physics Laws
A. Medium Invariance of Speed
Propagation speed $v$ is determined strictly by physical medium properties. $v_A = v_B$ in the same uniform medium.
B. Wave Relation & Pitch
$v = f \lambda \implies f = \frac{v}{\lambda}$
Human pitch perception depends directly on frequency $f$.
C. Intensity Law
For a mechanical/sound wave, intensity is $I = \frac{1}{2}\rho v \omega^2 A^2 \propto A^2 f^2$ (not amplitude alone). Intensity depends on the SQUARE of amplitude AND the SQUARE of frequency.
2. Analysis of Statements
- Statement III (Speed): Same uniform medium $\implies v_A = v_B \implies$ INCORRECT.
- Statement II (Pitch): $\lambda_A = \frac{1}{2} \lambda_B$ and $v_A = v_B \implies f_A = \frac{v_A}{\lambda_A} = \frac{v_B}{\lambda_B/2} = 2 f_B \implies$ higher pitch $\implies$ CORRECT.
- Statement I (Intensity): $I \propto A^2 f^2$. Amplitudes are equal, but $f_A = 2f_B$, so $\frac{I_A}{I_B} = \left(\frac{A_A}{A_B}\right)^2\left(\frac{f_A}{f_B}\right)^2 = 1^2 \times 2^2 = 4$. Wave A's intensity is 4x that of Wave B $\implies$ CORRECT.
3. Option Matching
Statements I and II are correct; III is false.
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. Only I — Incomplete Selection
Statement III is also needed: Statement II (pitch) is also correct, since Wave A's frequency is double Wave B's, so 'Only I' misses that. - B. Only II — Conceptual Misunderstanding
Assumes intensity depends only on amplitude, ignoring that intensity also scales with frequency squared ($I \propto A^2 f^2$). Since Wave A has double the frequency, its intensity is actually 4x greater, so Statement I is also true. - C. Only III — Conceptual Misunderstanding
The speeds are exactly equal because the medium is identical; Statement III is false, and this option also misses the two true statements (I and II). - E. II and III — Conceptual Misunderstanding
Statement III is false because wave speed is invariant in a uniform medium; this option incorrectly includes III and omits I.
Common Mistake (⚠️):
Believing intensity depends on amplitude ALONE (a common oversimplification). The correct relationship, $I \propto A^2 f^2$, means two waves of equal amplitude but different frequency do NOT have equal intensity. A student who stops at 'equal amplitude therefore equal intensity' will incorrectly mark Statement I as false and select Option B instead of D.
Takeaway (📌):
Wave speed depends on medium. Pitch depends on frequency. Intensity depends on BOTH amplitude and frequency ($I \propto A^2 f^2$), not amplitude alone.
Question 25
Back to top ↑Given two objects A and B with the specific heat capacities c and 3c and masses $2m$ and $m$ respectively, and assuming they are heated from temperature $T$ to $2T$, if the amount of heat received by object A is Q, what is the amount of heat received by object B?
Key Idea (💡): The heat energy received by an object is given by $Q = m c \Delta T$.
Reveal the answer & worked solution — commit to an option first
Correct Answer: C. 3Q/2
Fastest Approach (🚀):
For object A: $Q = 2 \ \text{m} \cdot c \cdot T = 2mcT$.
For object B: $Q_B = m \cdot 3c \cdot T = 3mcT$.
Ratio: $\frac{Q_B}{Q} = \frac{3mcT}{2mcT} = 1.5 \implies Q_B = \frac{3}{2}Q$.
Matches Option C.
Step-by-Step Breakdown:
1. Specific Heat Capacity Equation
The fundamental equation linking heat energy, mass, specific heat capacity, and temperature change is:
$Q = m \cdot c \cdot \Delta T$
Where:
- $Q$ is the heat energy transferred
- $m$ is the mass of the object
- $c$ is the specific heat capacity (energy required to raise 1 kg by 1 Kelvin)
- $\Delta T$ is the change in temperature
2. analysing Object A
- The mass is $m_A = 2m$.
- The specific heat capacity is $c_A = c$.
- The temperature changes from $T$ to $2T$, so $\Delta T = 2T - T = T$.
The heat received by object A is defined as $Q$.
Using our formula:
$Q_A = (2m) \cdot (c) \cdot (T) = 2mcT$
So we know that $Q = 2mcT$. We can rearrange this to find a useful substitution: $mcT = \frac{Q}{2}$.
3. analysing Object B
- The mass is $m_B = m$.
- The specific heat capacity is $c_B = 3c$.
- The temperature change is identical, $\Delta T = T$.
The heat received by object B is $Q_B$.
$Q_B = (m) \cdot (3c) \cdot (T) = 3mcT$
4. Final Ratio & Substitution
We need to express $Q_B$ in terms of the original $Q$.
Substitute our rearranged term $mcT = \frac{Q}{2}$ directly into the equation for $Q_B$:
$Q_B = 3(mcT) = 3 \left(\frac{Q}{2}\right) = \frac{3}{2} Q$
5. Option Matching
Matches Option C.
Why the Other Options Are Wrong (❌):
- A. Q — Incomplete Calculation
Forgetting to account for the differences in mass and specific heat between the two objects. - B. 2Q/3 — Unit Conversion Error
Inverting the final mathematical ratio. - D. 2Q — Incomplete Calculation
Making an arithmetic error during the substitution step. - E. 3Q — Conceptual Misunderstanding
Only comparing the specific heat capacities (3:1) and entirely ignoring the mass difference (1:2).
Common Mistake (⚠️):
Dividing specific heat values incorrectly, or only looking at the specific heat capacity ratio (3:1) and entirely forgetting to account for the difference in mass (1:2).
Takeaway (📌):
When comparing two thermal systems, calculate individual products of mass, specific heat, and temperature change for both, then find the relative ratio of their heat energy.
Question 26
Back to top ↑A nucleus emits alpha, beta, and gamma rays sequentially. Which of the following statements are correct? I. The resulting nucleus is the same element as the original nucleus. II. Electromagnetic waves are emitted. III. The energy of the nucleus decreases. IV. Of the three types of radiation, gamma rays have the greatest range in air.
Key Idea (💡): Spontaneous radioactive decays conserve mass and charge, releasing energy. Gamma rays are high-frequency electromagnetic radiation with high penetration depth.
Reveal the answer & worked solution — commit to an option first
Correct Answer: D. II, III, IV
Fastest Approach (🚀):
After $\alpha$ emission ($Z-2, A-4$), atomic number becomes $90$. After $\beta^-$ emission ($Z+1$), atomic number becomes $91$. Statement I is false.
Gamma rays are EM waves (II true). Decays release energy (III true). Gamma rays have greatest range in air (IV true).
Statements II, III, IV are correct.
Matches Option D.
Step-by-Step Breakdown:
1. Nuclear Transformation & Decay Particle Characteristics
- Alpha Emission: Helium nucleus ($^4_2 \text{He}$), $\Delta Z = -2, \Delta A = -4$.
- Beta-Minus Emission: Fast electron ($^0_{-1}\text{e}$), $\Delta Z = +1, \Delta A = 0$.
- Gamma Emission: High-frequency photon (EM wave), no mass or charge, high penetration/range.
2. Statement-by-Statement Verification
- Statement I (Turns into X Nucleus): Starting $Z, A$. After $\alpha$, $Z-2$. After $\beta$, $Z-2+1 = Z-1 ≠ Z \implies$ FALSE.
- Statement II (Electromagnetic Waves Emitted): Gamma rays are EM waves $\implies$ TRUE.
- Statement III (Nuclear Energy Decreases): Spontaneous decay releases energy to lower, more stable nuclear state $\implies$ TRUE.
- Statement IV (Gamma Greatest Range in Air): Neutral gamma photons interact less frequently with air molecules than charged $\alpha$ or $\beta$ particles $\implies$ greatest range $\implies$ TRUE.
3. Option Matching
Statements II, III, IV are correct.
Matches Option D.
Why the Other Options Are Wrong (❌):
- A. III and IV — Unit Conversion Error
Missing Statement II, which is also a scientifically correct statement. - B. I and III — Conceptual Misunderstanding
Statement I is false because beta decay changes the atomic number back to Z-1, not the original Z. - C. I, II and III — Conceptual Misunderstanding
Statement I is false for the reason above. - E. I, II, III, and IV — Conceptual Misunderstanding
Statement I is false for the reason above.
Common Mistake (⚠️):
Failing to apply the beta decay step to the atomic number, thereby assuming Statement I is correct.
Takeaway (📌):
analyse radioactive sequences step-by-step. Beta decay increases atomic number, which changes the chemical element.
Question 27
Back to top ↑One night, a careless driver crashes into a lamppost while driving at a speed of $108 \ \text{km/h}$. As a result of the collision the car comes to a stop after the front parts are compressed by $0.45 \ \text{m}$. What is the deceleration of the car? Assume the car's deceleration is constant.
Key Idea (💡): Use the constant acceleration kinematic formula $v^2 = u^2 + 2as$ to determine deceleration.
Reveal the answer & worked solution — commit to an option first
Correct Answer: A. $-1000 \ \text{m/s}^2$
Fastest Approach (🚀):
$u = 108 \ \text{km/h} = 30 \ \text{m/s}, s = 0.45 \ \text{m}$.
$a = -\frac{u^2}{2 \ \text{s}} = -\frac{900}{0.9} = -1000 \text{m s}^{-2}$.
Matches Option A.
Step-by-Step Breakdown:
1. Standardizing Units (Crucial First Step)
Before applying any kinematic equations, all values must be in standard SI units (metres and seconds). The initial speed $u$ is given in $\text{km/h}$.
To convert from $\text{km/h}$ to $\text{m/s}$, we divide by 3.6 (since there are 1000 metres in a kilometre and 3600 seconds in an hour, $1000/3600 = 1/3.6$).
$u = 108 \ \text{km/h} = \frac{108}{3.6} = 30 \ \text{m/s}$
2. Selecting the Correct SUVAT Equation
We need to find the constant deceleration ($a$). We know:
- Initial velocity $u = 30 \ \text{m/s}$
- Final velocity $v = 0 \ \text{m/s}$ (since the car comes to a stop)
- Displacement $s = 0.45 \ \text{m}$ (the compression distance of the car parts)
- Time $t$ is unknown and unneeded.
Because we have $u, v, s$ and want $a$, we use the time-independent kinematic equation:
$v^2 = u^2 + 2 a s$
3. Deceleration Calculation
Substitute the known values into the equation:
$0^2 = (30)^2 + 2 \cdot a \cdot (0.45)$
$0 = 900 + 0.9a$
Rearrange to solve for $a$:
$0.9a = -900$
$a = -\frac{900}{0.9}$
$a = -1000 \text{m s}^{-2}$
The negative sign perfectly indicates deceleration, exactly as expected for a collision.
4. Option Matching
Matches Option A.
Why the Other Options Are Wrong (❌):
- B. $-100 \ \text{m/s}^2$ — Unit Conversion Error
Using an incorrect speed conversion factor or making a decimal arithmetic error. - C. $-10 \ \text{m/s}^2$ — Unit Conversion Error
Making an order of magnitude error during the final division. - D. $-900 \ \text{m/s}^2$ — Misapplied Formula
Forgetting the factor of 2 in the kinematic equation (v^2 = u^2 + as). - E. $-90 \ \text{m/s}^2$ — Conceptual Misunderstanding
Forgetting the factor of 2 and making a decimal error.
Common Mistake (⚠️):
Plugging 108 directly into the SUVAT equation without converting it from km/h to m/s, which results in a wildly incorrect deceleration of $-12960 \text{m/s}^2$.
Takeaway (📌):
Always verify that your speed units are in standard SI metres per second (m/s) before applying equations of motion. If they are in km/h, divide by 3.6.