Motion and Forces

Topic 3: Motion and Forces

Course: Prep4Uni Physics 1

Chapter 1: Quantities and Measurement
Chapter 2: Forces and Moments
Chapter 3: Motion and Forces
Chapter 4: Energy and Fields
Chapter 5: Projectile Motion


🚁Overview

This topic develops your understanding of how and why objects move. It connects the description of motion (kinematics) with the forces that cause motion, using Newton’s Laws as a foundation for analyzing dynamics in real-world and theoretical situations.

📖Contents

  • Kinematics and uniformly accelerated motion
  • Linear momentum
  • Newton’s Laws of Motion

🎯Learning Outcomes

By the end of this section, students should be able to:

  • Define and use terms: displacement, speed, velocity, and acceleration
  • Use and interpret motion-time and velocity-time graphs
  • Derive and apply the kinematic equations for uniformly accelerated motion
  • Understand mass as a measure of inertia
  • Define and use momentum in practical situations
  • Apply Newton’s Laws to explain and predict motion
  • Solve problems using Newton’s Second Law: F = ma

Table of Contents

🔢1. Kinematics and Uniformly Accelerated Motion

Key concepts.
  • Displacement \( (s) \): change in position (vector; includes direction).
  • Speed \( (v) \): scalar rate of motion; \( v=\frac{\text{distance}}{\text{time}} \).
  • Velocity \( (v) \): vector rate of change of position (magnitude + direction).
  • Acceleration \( (a) \): rate of change of velocity; \( a=\frac{\Delta v}{\Delta t} \).
Equations of motion (constant acceleration).
  • \( v = u + a t \)   (vector form: \( \vec v=\vec u+\vec a\,t \)).
  • \( s = u t + \frac12 a t^{2} \)   (area under the \(v\)-\(t\) graph).
  • \( v^{2} = u^{2} + 2 a s \)   (useful when time \( t \) is unknown).
Symbols: \( u \) = initial velocity, \( v \) = final velocity, \( a \) = acceleration, \( s \) = displacement, \( t \) = time.

Vector relation v = u + at

Vector relation: \( \vec v = \vec u + \vec a\,t \).

Displacement as area under a velocity–time graph

Displacement from \( v\!-\!t \) graph: \( s = u t + \frac12 a t^{2} \).

Illustration of v² = u² + 2as

When \( t \) is unknown: \( v^{2} = u^{2} + 2 a s \).

Worked example. A car accelerates from \(10~\text{m s}^{-1}\) to \(30~\text{m s}^{-1}\) in \(5~\text{s}\). Find its acceleration.
  • Use \( a=\frac{v-u}{t} \).
  • \( a=\frac{30-10}{5}=4~\text{m s}^{-2}. \)

Answer: \( 4~\text{m s}^{-2} \).

📐 Learning-Check 1. A ball is thrown upward at \(15~\text{m s}^{-1}\). How long until it reaches its highest point?
  • At the top, \( v=0 \). Take upward \( + \), use \( a=-g\approx-9.8~\text{m s}^{-2} \).
  • \( t=\frac{v-u}{a}=\frac{0-15}{-9.8}\approx 1.53~\text{s}. \)

Answer: \( \approx 1.53~\text{s} \).

📐 Learning-Check 2. A train accelerates uniformly from rest to \(25~\text{m s}^{-1}\) in \(10~\text{s}\). Find the displacement in this time.
  • First \( a=\frac{25-0}{10}=2.5~\text{m s}^{-2} \).
  • Then \( s=u t+\frac12 a t^{2}=0+\frac12(2.5)(10^{2})=125~\text{m}. \)

Answer: \( 125~\text{m} \).

Exam tip: choose a clear sign convention (e.g., upward \(+\)) and stick to it; check units at each step (\(\text{m}, \text{s}, \text{m s}^{-1}, \text{m s}^{-2}\)).

🔢2. Interpreting Motion Graphs

Displacement–time graph (s–t).
  • Slope = instantaneous velocity: \( v=\frac{\Delta s}{\Delta t} \) for a straight segment, \( v(t)=\frac{ds}{dt} \) in general.
  • Horizontal line ⇒ \( v=0 \) (object at rest). Steeper line ⇒ larger speed.
  • Positive slope ⇒ motion in + direction; negative slope ⇒ motion in − direction.
Example displacement–time graph; slope at any point equals velocity
Displacement–time: slope gives velocity.
Velocity–time graph (v–t).
  • Slope = acceleration: \( a=\frac{\Delta v}{\Delta t} \) for a straight segment, \( a(t)=\frac{dv}{dt} \) in general.
  • Area under the curve = displacement over an interval: \( s=\int_{t_1}^{t_2} v(t)\,dt \).
  • Horizontal line ⇒ constant velocity (\( a=0 \)). A rising line through \( v=0 \) ⇒ speeding up in the + direction.
Example velocity–time graph; slope equals acceleration and area equals displacement
Velocity–time: slope gives acceleration; area gives displacement.
Worked example. A v–t graph is a straight line from \( v=0 \) at \( t=0 \) to \( v=20~\text{m s}^{-1} \) at \( t=4~\text{s} \).
  • Acceleration (slope): \( a=\frac{\Delta v}{\Delta t}=\frac{20-0}{4-0}=5~\text{m s}^{-2} \).
  • Displacement (area of triangle): \( s=\frac12\times\text{base}\times\text{height}=\frac12\times 4\times 20=40~\text{m} \).

Answer: \( a=5~\text{m s}^{-2} \), \( s=40~\text{m} \).

Quick checks. On an s–t graph, upward curvature (slope increasing) ⇒ \( a>0 \); downward curvature ⇒ \( a<0 \). On a v–t graph, the signed area (above positive, below negative) gives signed displacement.
📐 Learning-Check 1. On a v–t graph, what does a horizontal line represent?

Answer: Constant velocity (\( a=0 \)).

📐 Learning-Check 2. What physical quantity is the area under a v–t graph?

Answer: Displacement over that time interval, \( s=\int v(t)\,dt \).

🔢3. Newton’s Laws of Motion

First Law (Inertia): A body remains at rest or moves with constant velocity when the net external force is zero. In symbols: \( \sum \vec F = \vec 0 \Rightarrow \vec v = \text{constant} \).

Second Law (Dynamics): Net force equals mass times acceleration: \( \sum \vec F = m\,\vec a \). More generally, \( \sum \vec F = \frac{d\vec p}{dt} \) with momentum \( \vec p = m\vec v \) (for constant \( m \Rightarrow m\,\vec a \)).

Third Law (Action–Reaction): Forces between two bodies are equal in magnitude and opposite in direction: \( \vec F_{A\to B} = -\,\vec F_{B\to A} \). They act on different bodies and therefore do not cancel in a single free-body diagram.

Units & components: \( [\vec F] = \text{kg m s}^{-2} = \text{N} \). Components: \( \sum F_x = m a_x,\ \sum F_y = m a_y \). Weight: \( W = m g \) (near Earth, \( g \approx 9.8~\text{m s}^{-2} \)).

Worked example. A \(3.0~\text{kg}\) object accelerates at \(2.0~\text{m s}^{-2}\) in the \(+x\) direction. Find the net force.
  • By the second law: \( F_{\text{net}} = m a = 3.0 \times 2.0 = 6.0~\text{N} \) in \(+x\).
  • If several forces act (e.g., push \(P\) and friction \(f\)), then \( P – f = 6.0~\text{N} \). Knowing either \(P\) or \(f\) lets you solve for the other.

Answer: \( 6.0~\text{N} \) along \(+x\).

📐 Learning-Check 1. A box is pushed with \(10~\text{N}\) on frictionless ice and accelerates at \(5.0~\text{m s}^{-2}\). What is its mass?

\( m = \frac{F}{a} = \frac{10}{5.0} = 2.0~\text{kg} \).

📐 Learning-Check 2. Which law explains why passengers lurch forward when a car stops suddenly?

Newton’s First Law (Inertia) — bodies tend to maintain their current state of motion.

Common pitfalls. (i) Treating action–reaction forces as if they act on the same object (they don’t). (ii) Forgetting to resolve forces before using \( \sum F_x = m a_x \), \( \sum F_y = m a_y \). (iii) Confusing mass (kg) with weight (N).
Illustration Video:

🔢4. Mass and Inertia

Mass (m) quantifies an object’s resistance to changes in its motion (inertia). For a given net force, acceleration is smaller when mass is larger: \( \vec a = \frac{\sum \vec F}{m} \).

Inertia is the tendency to maintain the current state of motion (rest or constant velocity). More mass ⟹ more inertia ⟹ harder to start/stop/turn.

Units & types of mass. SI unit: kilogram (kg). In everyday mechanics we treat inertial mass (resists acceleration) and gravitational mass (appears in \( W = m g \)) as numerically identical.

Mass vs weight. Mass (kg) is intrinsic; weight is a force: \( W = m g \) (newtons). On the Moon, \(g\) is smaller, so weight changes while mass stays the same.

Worked example. Two carts are pushed by the same horizontal force \( F = 12~\text{N} \). Cart A has \( m_A = 3.0~\text{kg} \); Cart B has \( m_B = 6.0~\text{kg} \).
  • Cart A: \( a_A = \frac{F}{m_A} = \frac{12}{3.0} = 4.0~\text{m s}^{-2} \).
  • Cart B: \( a_B = \frac{F}{m_B} = \frac{12}{6.0} = 2.0~\text{m s}^{-2} \).
  • Conclusion: the lighter cart accelerates twice as much under the same force (less inertia).

Answer: \( a_A = 4.0~\text{m s}^{-2} \), \( a_B = 2.0~\text{m s}^{-2} \).

📐 Learning-Check 1. Two carts, one light and one heavy, are pushed with equal force. Which accelerates more, and why?

The lighter cart. From \( a = \frac{F}{m} \), smaller \(m\) gives larger \(a\) (less inertia).

📐 Learning-Check 2. What physical property resists changes in velocity? Give its SI unit and a common equation where it appears.

Inertia (quantified by mass, unit kg). It appears in \( \sum \vec F = m \vec a \) and \( W = m g \).

Exam tip. When comparing situations, keep either the force or the acceleration fixed and vary the other with \( \sum \vec F = m\vec a \). Also check units: mass in kg, weight in newtons.

🔢5. Linear Momentum

Definition (vector): linear momentum \( \vec p \) is \( \vec p = m\,\vec v \). Unit: kg·m·s\(^{-1}\).

Impulse–momentum theorem: The impulse delivered by a net force equals the change in momentum: \[ \vec J \equiv \int_{t_1}^{t_2} \vec F_{\text{net}}(t)\,dt = \Delta \vec p = \vec p_2 – \vec p_1. \] For an approximately constant force over \(\Delta t\): \( \vec F_{\text{avg}} = \frac{\Delta \vec p}{\Delta t} \).

Newton’s 2nd Law (momentum form): \( \vec F_{\text{net}} = \frac{d\vec p}{dt} \). For constant mass, \( \vec F_{\text{net}} = m\,\vec a \).

Conservation of momentum: In an isolated system (external net impulse \(= \vec 0\)), total momentum is conserved: \[ \sum \vec p_{\text{initial}} = \sum \vec p_{\text{final}}. \] Energy may or may not be conserved (elastic vs inelastic collisions).

Impulse changes momentum: area under force–time equals Δp
Impulse changes momentum: area under \(F\)–\(t\) equals \(\Delta p\).
Worked example 1 (wall impact). A \(2.0~\text{kg}\) trolley moves at \(+3.0~\text{m s}^{-1}\), hits a wall, and stops in \(0.10~\text{s}\).
  • Initial momentum: \( \vec p_i = (2.0)(+3.0) = +6.0~\text{kg m s}^{-1} \).
  • Final momentum: \( \vec p_f = 0 \Rightarrow \Delta \vec p = \vec p_f – \vec p_i = -6.0~\text{kg m s}^{-1} \) (opposite motion).
  • Average force on trolley: \( \vec F_{\text{avg}} = \frac{\Delta \vec p}{\Delta t} = \frac{-6.0}{0.10} = -60~\text{N} \) (direction opposite the incoming motion).

Report: magnitude \(60~\text{N}\), directed opposite to the initial velocity.

Worked example 2 (1-D inelastic collision). A \(0.40~\text{kg}\) cart moving at \(+2.5~\text{m s}^{-1}\) sticks to a \(0.60~\text{kg}\) cart at rest. Find the common speed immediately after they stick.
  • Before: \( p_i = (0.40)(+2.5) + (0.60)(0) = +1.00~\text{kg m s}^{-1} \).
  • After (stuck): total mass \(= 1.00~\text{kg}\), speed \(v_f\) so \( p_f = (1.00)v_f \).
  • Conservation: \( p_f = p_i \Rightarrow v_f = \frac{1.00}{1.00} = 1.00~\text{m s}^{-1} \) (to the right).

Answer: \( v_f = 1.00~\text{m s}^{-1} \) (perfectly inelastic; kinetic energy is not conserved).

📐 Learning-Check 1. A \(0.50~\text{kg}\) ball rolls at \(8.0~\text{m s}^{-1}\). What is its momentum?

\( p = m v = 0.50 \times 8.0 = 4.0~\text{kg m s}^{-1} \) (direction of motion).

📐 Learning-Check 2. A constant force of \(20~\text{N}\) acts for \(0.20~\text{s}\) on a puck initially at rest. What impulse is delivered and what final speed does a \(0.40~\text{kg}\) puck reach?

Impulse: \( J = F\,\Delta t = 20 \times 0.20 = 4.0~\text{N s} = 4.0~\text{kg m s}^{-1} \).
Final speed: \( v = \frac{\Delta p}{m} = \frac{4.0}{0.40} = 10~\text{m s}^{-1} \).

⚙️Key Concepts Recap

Core relations (constant-acceleration kinematics, Newton’s laws, and momentum)
ConceptFormulaWhen / notes
Displacement (s)\( s = u t + \frac{1}{2} a t^{2} \)Uniform acceleration; area under \(v\)–\(t\) graph.
Final velocity (v)\( v = u + a t \)Vector form: \( \vec v = \vec u + \vec a\,t \).
Time-free kinematic\( v^{2} = u^{2} + 2 a s \)Use when \(t\) is unknown.
Average acceleration\( a_{\text{avg}}=\frac{\Delta v}{\Delta t} \)Slope of \(v\)–\(t\) graph on straight segments.
Displacement from \(v\)–\(t\)\( s = \int_{t_1}^{t_2} v(t)\,dt \)Area under the \(v\)–\(t\) curve; sign matters.
Newton’s 2nd Law\( \sum \vec F = m\,\vec a \)Momentum form: \( \sum \vec F = \frac{d\vec p}{dt} \).
Weight\( W = m g \)Near Earth, \( g \approx 9.8~\text{m s}^{-2} \).
Linear momentum\( \vec p = m\,\vec v \)Unit: kg·m·s\(^{-1}\); vector quantity.
Impulse\( \vec J=\int \vec F\,dt=\Delta \vec p \)For constant \(F\): \( \vec J=\vec F\,\Delta t \).

Additional Resources:

To deepen your understanding, you are strongly encouraged to explore the materials provided on the following pages.

EXERCISES

25 Learning-Check Questions & Answers
(5 from each of the 5 subsections in “Motion and Forces”)


Section 1: Displacement, Speed, Velocity & Acceleration
  1. Q: What is the difference between distance and displacement?
    A: Distance is total path length (scalar). Displacement is straight-line change from start to finish (vector with direction).
  2. Q: A runner goes 200 m east then 150 m west. What are the total distance and displacement?
    A: Distance \(=200+150=350~\text{m}\). Displacement \(=200-150=50~\text{m}\) east.
  3. Q: Define speed and instantaneous velocity.
    A: Speed \(=\frac{\text{distance}}{\text{time}}\) (scalar). Instantaneous velocity \(=\frac{d\vec s}{dt}\) (vector rate of change of position).
  4. Q: A car covers \(180~\text{km}\) north in \(3~\text{h}\), then \(60~\text{km}\) east in \(1~\text{h}\). Find the average velocity vector (magnitude & direction).
    A: Displacement \(=(60,\,180)~\text{km}\). Total time \(=4~\text{h}\).
    Magnitude \(=\frac{\sqrt{60^{2}+180^{2}}}{4}=\frac{189.74}{4}\approx 47.4~\text{km h}^{-1}\).
    Direction \(=\arctan\!\big(\frac{180}{60}\big)\approx 71.6^\circ\) north of east.
  5. Q: What is the physical meaning of a negative acceleration?
    A: The velocity’s magnitude decreases (deceleration) or the velocity is directed opposite the chosen positive direction.

Section 2: Motion Graphs
  1. Q: On a displacement–time (s–t) graph, how do you tell if an object is accelerating?
    A: Non-linear (curved) graph ⇒ slope changes with time ⇒ acceleration present.
  2. Q: On a velocity–time (v–t) graph, what does the area under the curve represent?
    A: Displacement over that interval: \( s=\int v(t)\,dt\).
  3. Q: A v–t graph is a straight line from \((0,0)\) to \((5~\text{s},\,20~\text{m s}^{-1})\). What are the acceleration and distance traveled?
    A: \(a=\frac{\Delta v}{\Delta t}=\frac{20}{5}=4~\text{m s}^{-2}\). Distance \(=\frac12\times 5\times 20=50~\text{m}\). → Using \(\frac12\) as \(\frac12\).
  4. Q: What feature of a v–t graph indicates constant velocity?
    A: A horizontal line (zero slope ⇒ \(a=0\)).
  5. Q: How do you find instantaneous acceleration on an s–t graph?
    A: Acceleration \(= \frac{d^{2}s}{dt^{2}}\) (concavity). Upward curvature ⇒ \(a>0\).

Section 3: Uniformly Accelerated Motion
  1. Q: State the three “suvat” equations for constant acceleration.
    A: \(v=u+at\);   \(s=ut+\frac12 at^{2}\);   \(v^{2}=u^{2}+2as\).
  2. Q: Derive \(s=\frac12 a t^{2}\) for motion from rest.
    A: With \(u=0\): \(s=ut+\frac12 at^{2}=0+\frac12 at^{2}\).
  3. Q: How long does a stone dropped from rest take to fall \(20~\text{m}\) ( \(g=9.8~\text{m s}^{-2}\) )?
    A: \(s=\frac12 g t^{2}\Rightarrow t=\sqrt{\frac{2s}{g}}=\sqrt{\frac{40}{9.8}}\approx 2.02~\text{s}\).
  4. Q: A car accelerates uniformly from \(10\) to \(30~\text{m s}^{-1}\) over \(50~\text{m}\). Find \(a\).
    A: \(v^{2}=u^{2}+2as\Rightarrow 30^{2}=10^{2}+2a(50)\Rightarrow a=8~\text{m s}^{-2}\).
  5. Q: If \(a=0\), which kinematic equations still hold?
    A: \(v=u\) (constant), \(s=ut\), and \(v^{2}=u^{2}\).

Section 4: Linear Momentum
  1. Q: Define linear momentum and its SI unit.
    A: \(\vec p = m\vec v\). Unit: \(\text{kg·m s}^{-1}\).
  2. Q: What is impulse, and how is it related to momentum?
    A: Impulse \(J=\vec F\,\Delta t\); \(J=\Delta \vec p\).
  3. Q: A \(0.5~\text{kg}\) ball thrown at \(20~\text{m s}^{-1}\) has what momentum?
    A: \(p=0.5\times 20=10~\text{kg·m s}^{-1}\).
  4. Q: A constant \(5~\text{N}\) force acts for \(3~\text{s}\) on a \(1~\text{kg}\) mass initially at rest. What is the final speed?
    A: \(J=5\times 3=15~\text{N·s}=\Delta p=m\,\Delta v\Rightarrow v=15/1=15~\text{m s}^{-1}\).
  5. Q: State conservation of momentum for a closed system.
    A: Total momentum before \(=\) total momentum after, if no external forces act.

Section 5: Newton’s Laws of Motion
  1. Q: State Newton’s First Law.
    A: A body remains at rest or moves with constant velocity unless acted upon by a net external force.
  2. Q: Give a real-world example of Newton’s First Law.
    A: A hockey puck glides on nearly frictionless ice at constant speed in a straight line.
  3. Q: State Newton’s Second Law.
    A: \(\sum \vec F = m\,\vec a\).
  4. Q: What is the reaction force to the weight of a book on a table (Third Law)?
    A: The book exerts an equal-and-opposite downward force on the table.
  5. Q: A \(5~\text{kg}\) block is pushed with \(20~\text{N}\) across a frictionless floor. What is its acceleration?
    A: \(a=\frac{F}{m}=\frac{20}{5}=4~\text{m s}^{-2}\).

Tip: Keep a consistent sign convention, write units at each step, and check vector directions before substituting numbers.

20 Problems with Detailed Solutions
(Covering all five sections of “Motion and Forces”)


Section 1: Displacement & Kinematics

  1. Variable-Speed Journey

    A car’s velocity is \(v(t)=4t\) (m/s) for \(0\le t\le 5\ \text{s}\).

    a) Displacement from \(t=0\) to \(5\ \text{s}\).

    b) Acceleration at \(t=2\ \text{s}\).

    Solution.
    a) \( s=\int_{0}^{5} 4t\,dt=[2t^{2}]_{0}^{5}=50~\text{m}.\)
    b) \( a=\frac{dv}{dt}=4~\text{m s}^{-2}\) (constant).
  2. Change of Direction

    A cyclist travels \(100~\text{m}\) east in \(20~\text{s}\), then \(60~\text{m}\) west in \(15~\text{s}\).

    a) Total distance and displacement.

    b) Average speed and average-velocity magnitude.

    Solution.
    a) Distance \(=160~\text{m}\); Displacement \(=100-60=40~\text{m}\) east.
    b) \(\text{Avg speed}=160/35\approx 4.57~\text{m s}^{-1}\);
    \(\ |\vec v_{\text{avg}}|=40/35\approx 1.14~\text{m s}^{-1}\) east.
  3. Instantaneous vs. Average

    A particle’s position is \(s(t)=t^{3}-6t^{2}+9t\) (m).

    a) Average velocity on \(t\in[1,3]\).

    b) Instantaneous velocity at \(t=2~\text{s}\).

    Solution.
    a) \(s(3)=0,\ s(1)=4 \Rightarrow \Delta s=-4,\ \Delta t=2\Rightarrow v_{\text{avg}}=-2~\text{m s}^{-1}.\)
    b) \(v(t)=3t^{2}-12t+9\Rightarrow v(2)=-3~\text{m s}^{-1}.\)
  4. Non-Uniform Motion

    A runner’s speed increases uniformly from \(5\) to \(9~\text{m s}^{-1}\) in \(4~\text{s}\), then remains constant.

    a) Sketch \(v\)–\(t\). b) Distance in first \(4~\text{s}\) and next \(6~\text{s}\).

    Solution.
    a) Line from \((0,5)\) to \((4,9)\), then horizontal at \(v=9\).
    b) First \(4~\text{s}\): trapezoid area \(=\frac{(5+9)}{2}\cdot 4=28~\text{m}\). Next \(6~\text{s}\): \(9\cdot 6=54~\text{m}\).
  5. Rapid Deceleration

    A car at \(25~\text{m s}^{-1}\) brakes with constant \(a=-5~\text{m s}^{-2}\).

    a) Time to stop. b) Braking distance.

    Solution.
    a) \(0=u+at\Rightarrow t=25/5=5~\text{s}\).
    b) \(s=ut+\frac12 a t^{2}=25\cdot 5+\frac12(-5)\cdot 25=62.5~\text{m}\).

Section 2: Motion Graphs

  1. Piecewise \(v\)–\(t\) Analysis

    Given \(v\)–\(t\): \(0\!\to\!4~\text{s}\) at \(2\) m/s; \(4\!\to\!6~\text{s}\) linear to \(6\) m/s; \(6\!\to\!10~\text{s}\) constant at \(6\) m/s. Find total displacement.

    Solution. Areas: \(0\)–\(4\): \(2\cdot 4=8\). \(4\)–\(6\): trapezoid \(=\frac{2+6}{2}\cdot 2=8\). \(6\)–\(10\): \(6\cdot 4=24\). Total \(=40~\text{m}\).
  2. Reading \(s\)–\(t\) Curves

    \(s(t)=2t^{2}\).

    a) \(v\) at \(t=3~\text{s}\). b) \(a\).

    Solution. \(v=\frac{ds}{dt}=4t\Rightarrow v(3)=12~\text{m s}^{-1}\). \(a=\frac{dv}{dt}=4~\text{m s}^{-2}\).
  3. Acceleration–Time to Velocity

    An \(a\)–\(t\) graph is horizontal at \(a=3~\text{m s}^{-2}\) from \(0\) to \(5~\text{s}\). If \(u=2~\text{m s}^{-1}\), find \(v(t)\) and distance traveled.

    Solution. \(v(t)=u+at=2+3t\). Distance \(=\int_{0}^{5}(2+3t)\,dt=[2t+1.5t^{2}]_{0}^{5}=47.5~\text{m}\).
  4. Slope of \(s\)–\(t\)

    Line through \((2,6~\text{m})\) and \((5,15~\text{m})\). What is the speed?

    Answer. \(\text{slope}=\Delta s/\Delta t=(15-6)/(5-2)=3~\text{m s}^{-1}\).
  5. Curved vs. Straight

    Explain why a curved \(s\)–\(t\) graph always implies non-zero acceleration.

    Answer. Because the slope (velocity) changes with time \(\Rightarrow \frac{d^{2}s}{dt^{2}}\neq 0\).

Section 3: Uniformly Accelerated Motion

  1. Uphill Skate

    A skateboarder goes up a \(5~\text{m}\) slope with \(u=6~\text{m s}^{-1}\), coming to rest halfway. Find \(a\).

    Solution. Over \(s=2.5~\text{m}\): \(0=u^{2}+2as\Rightarrow a=-\frac{36}{5}=-7.2~\text{m s}^{-2}\).
  2. Downward Throw

    A stone is thrown downward at \(5~\text{m s}^{-1}\) from \(20~\text{m}\). Time to hit ground?

    Solution. \(s=ut+\frac12 gt^{2}\Rightarrow 20=5t+4.9t^{2}\Rightarrow t\approx 1.57~\text{s}\).
  3. Upward Launch

    A football is kicked at \(15~\text{m s}^{-1}\) upward.

    a) Time to max height. b) Max height.

    Solution. a) \(t=\frac{u}{g}=\frac{15}{9.8}\approx 1.53~\text{s}\).
    b) \(s_{\max}=\frac{u^{2}}{2g}=\frac{225}{19.6}\approx 11.48~\text{m}\).
  4. Braking Distance

    A car at \(20~\text{m s}^{-1}\) decelerates at \(4~\text{m s}^{-2}\). How far to stop?

    Solution. \(0=u^{2}+2as\Rightarrow s=\frac{u^{2}}{2|a|}=\frac{400}{8}=50~\text{m}\).
  5. Mid-race Speed

    From rest, \(a=3~\text{m s}^{-2}\) for \(8~\text{s}\), then coast. Speed at \(t=8~\text{s}\)?

    Answer. \(v=at=3\cdot 8=24~\text{m s}^{-1}\).

Section 4: Linear Momentum

  1. Crash Test

    A \(1000~\text{kg}\) car at \(20~\text{m s}^{-1}\) stops in \(0.1~\text{s}\). Average force on barrier?

    Solution. \(\Delta p=1000\cdot 20=2.0\times 10^{4}\). \(F_{\text{avg}}=\Delta p/\Delta t=2.0\times 10^{5}~\text{N}\).
  2. Recoil of Gun

    A \(0.01~\text{kg}\) bullet leaves a \(5~\text{kg}\) rifle at \(400~\text{m s}^{-1}\). Recoil speed?

    Solution. \(0=m_R v_R+m_b v_b\Rightarrow v_R=-(0.01\cdot 400)/5=-0.8~\text{m s}^{-1}\).
  3. Two-Mass Collision

    \(m_1=2~\text{kg}\) at \(u_1=3~\text{m s}^{-1}\) hits \(m_2=1~\text{kg}\) at rest, elastically. Speeds after?

    Solution.
    \(v_1’=\frac{m_1-m_2}{m_1+m_2}u_1=\frac{1}{3}\cdot 3=1~\text{m s}^{-1}\).
    \(v_2’=\frac{2m_1}{m_1+m_2}u_1=\frac{4}{3}\cdot 3=4~\text{m s}^{-1}\).
  4. Inelastic Impact

    A \(0.2~\text{kg}\) ball at \(5~\text{m s}^{-1}\) sticks to a \(0.8~\text{kg}\) block at rest. Final velocity?

    Solution. \(v=\frac{0.2\cdot 5 + 0}{1.0}=1.0~\text{m s}^{-1}\).
  5. Rocket Propulsion (Simplified)

    A rocket ejects \(100~\text{kg}\) of gas at \(2000~\text{m s}^{-1}\). Initial mass \(1000~\text{kg}\). \(\Delta v\)?

    Solution (Tsiolkovsky). \(\Delta v=v_e\ln\!\left(\frac{m_0}{m_1}\right)=2000\ln(1000/900)\approx 210.6~\text{m s}^{-1}\).

Section 5: Newton’s Laws

  1. Atwood Machine

    \(m_1=5~\text{kg},\ m_2=3~\text{kg}\) over a frictionless pulley. Find \(a\) and \(T\).

    Solution. \(a=\frac{(m_1-m_2)g}{m_1+m_2}=\frac{2\cdot 9.8}{8}=2.45~\text{m s}^{-2}\).
    \(T=m_1(g-a)=5(9.8-2.45)=\mathbf{36.75~\text{N}}\).
  2. Block on Incline with Friction

    \(m=4~\text{kg},\ \theta=30^\circ,\ \mu_k=0.20\). Find \(a\) down the slope.

    Solution.
    \(F_{\parallel}=mg\sin\theta=4\cdot 9.8\cdot 0.5=19.6~\text{N}\).
    \(f_k=\mu_k N=\mu_k mg\cos\theta=0.20\cdot 4\cdot 9.8\cdot 0.866\approx 6.79~\text{N}\).
    Net \(=19.6-6.79=12.81~\text{N}\Rightarrow a=12.81/4\approx \mathbf{3.20~\text{m s}^{-2}}\).
  3. Centripetal Force

    A \(0.5~\text{kg}\) mass on a \(2~\text{m}\) string circles at \(2~\text{rev s}^{-1}\). Tension?

    Solution. \(\omega=2(2\pi)=4\pi\ \text{rad s}^{-1}\).
    \(F=m\omega^{2}r=0.5(4\pi)^{2}\cdot 2=16\pi^{2}\approx 158~\text{N}\).
  4. Elevator Tension

    Elevator \(m=600~\text{kg}\) accelerates upward at \(1.5~\text{m s}^{-2}\). Cable tension?

    Solution. \(T-mg=ma\Rightarrow T=m(g+a)=600(9.8+1.5)=\mathbf{6780~\text{N}}\).
  5. Forced Oscillation (Hooke + Newton)

    Mass \(m=0.5~\text{kg}\) on spring \(k=100~\text{N m}^{-1}\) pulled to \(x=0.1~\text{m}\) and released. Max acceleration?

    Solution. \(a_{\max}=\frac{k}{m}x=\frac{100}{0.5}\cdot 0.1=20~\text{m s}^{-2}\).

Have feedback or questions? We’d love to hear from you!

Course: Prep4Uni Physics 1

Chapter 1: Quantities and Measurement
Chapter 2: Forces and Moments
Chapter 3: Motion and Forces
Chapter 4: Energy and Fields
Chapter 5: Projectile Motion

Last updated: 13 Nov 2025