๐ŸŽ Forces and Newton's Laws

A Level Maths Year 1 ยท Mechanics

Level 3 · Ages 16–17

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1 Forces and Force Diagrams

Kinematics describes motion; dynamics explains it. A force is a push or pull, measured in newtons (N), and it is a vector (DfE content area R ยท Forces and Newton's laws).

ForceSymbolWhere it acts and which way
Weight$W = mg$Vertically downwards, from the centre of mass.
Normal reaction$R$Perpendicular to a surface, pushing the object away from it.
Tension$T$Along a taut string or rod, pulling away from the object.
Thrust (compression)$T$Along a rod, pushing towards the object.
Friction$F$Along a rough surface, opposing motion (or attempted motion).
Driving force / resistance$D$, $R$Forward force from an engine; resistance opposes motion.
A force diagram shows the object (as a dot or a box) and every force acting on it, each as a labelled arrow. Show the acceleration separately with a double-headed arrow. Never include forces that the object exerts on other things.
Resolve in a direction: add the components of all forces in that direction, taking one way as positive. For now, every force is horizontal or vertical (or given in $\mathbf{i}$, $\mathbf{j}$ form), so there is no trigonometry โ€” that comes in Year 2.
2 Newton's Three Laws
Newton's laws of motion
1st: A body stays at rest or moves with constant velocity unless a resultant force acts on it.
2nd: Resultant force $=$ mass ร— acceleration:  $\mathbf{F} = m\mathbf{a}$
3rd: If body $A$ exerts a force on body $B$, then $B$ exerts an equal and opposite force on $A$.
Equilibrium means the resultant force is zero. By the first law, a particle in equilibrium is either at rest or moving with constant velocity โ€” both count.
Worked Example 1 โ€” F = ma in one dimension

A box of mass $4$ kg is pushed across a floor by a horizontal force of $30$ N against a resistance of $12$ N. Find its acceleration and the normal reaction.

โ‘ Horizontally ($\rightarrow$ positive): $30 - 12 = 4a \Rightarrow a = 4.5$ m s$^{-2}$.
โ‘กVertically, no acceleration: $R - 4g = 0 \Rightarrow R = 39.2$ N.
Worked Example 2 โ€” A particle on a string

A particle of mass $2$ kg hangs on a light string and is pulled upwards with tension $26$ N. Find its acceleration.

โ‘ Up positive: $26 - 2g = 2a$.
โ‘ก$26 - 19.6 = 6.4 = 2a \Rightarrow a = 3.2$ m s$^{-2}$ upwards.
Weight and normal reaction are not a third-law pair. Both act on the same object. The third-law partner of the box's weight is the box's gravitational pull on the Earth; the partner of the normal reaction is the box pushing down on the floor.
3 Forces as Vectors

When forces are given in $\mathbf{i}$, $\mathbf{j}$ form, add them component by component (see Vectors in Two Dimensions). Newton's second law applies to each component separately.

In two dimensions
$\mathbf{F}_1 + \mathbf{F}_2 + \cdots = m\mathbf{a}$;   equilibrium $\iff$ $\sum \mathbf{F} = \mathbf{0}$
Worked Example 3 โ€” Acceleration from vector forces

Forces $(3\mathbf{i} + 4\mathbf{j})$ N and $(5\mathbf{i} - 10\mathbf{j})$ N act on a particle of mass $2$ kg. Find its acceleration and the magnitude of the acceleration.

โ‘ Resultant $= (8\mathbf{i} - 6\mathbf{j})$ N.
โ‘ก$\mathbf{a} = \dfrac{1}{2}(8\mathbf{i} - 6\mathbf{j}) = (4\mathbf{i} - 3\mathbf{j})$ m s$^{-2}$.
โ‘ข$|\mathbf{a}| = \sqrt{16 + 9} = 5$ m s$^{-2}$.
Worked Example 4 โ€” Equilibrium

Forces $(2\mathbf{i} - 3\mathbf{j})$, $(-5\mathbf{i} + q\mathbf{j})$ and $(p\mathbf{i} + 7\mathbf{j})$ N act on a particle in equilibrium. Find $p$ and $q$.

โ‘ $\mathbf{i}$: $2 - 5 + p = 0 \Rightarrow p = 3$.
โ‘ก$\mathbf{j}$: $-3 + q + 7 = 0 \Rightarrow q = -4$.
4 Connected Particles: Lifts
For connected objects that move together, you can apply $F = ma$ to the whole system (internal forces cancel) or to each part separately (internal forces appear). Use whichever gives the unknown you want most directly โ€” and use the other as a check.
Worked Example 5 โ€” Person in a lift

A lift of mass $430$ kg carries a man of mass $70$ kg. It accelerates upwards at $0.5$ m s$^{-2}$. Find the tension in the lift cable and the normal reaction of the floor on the man.

โ‘ Whole system ($500$ kg), up positive: $T - 500g = 500(0.5)$.
โ‘ก$T = 4900 + 250 = 5150$ N.
โ‘ขMan alone: $R - 70g = 70(0.5) \Rightarrow R = 686 + 35 = 721$ N.
$R$ is greater than his weight ($686$ N): he feels heavier while the lift accelerates upwards. When it decelerates on the way up, $R$ is less than $686$ N.
5 Connected Particles: Cars and Trailers

A car and trailer are joined by a light, rigid towbar. When the car pulls, the towbar is in tension; when the car brakes, the trailer pushes on it and the towbar is in thrust.

Worked Example 6 โ€” Tension in a towbar

A car of mass $1200$ kg tows a trailer of mass $400$ kg along a straight horizontal road. The engine's driving force is $2500$ N; resistances are $300$ N on the car and $200$ N on the trailer. Find the acceleration and the tension in the towbar.

โ‘ Whole system: $2500 - 300 - 200 = 1600a \Rightarrow a = 1.25$ m s$^{-2}$.
โ‘กTrailer alone: $T - 200 = 400(1.25) \Rightarrow T = 700$ N.
โ‘ขCheck with the car: $2500 - 300 - 700 = 1500 = 1200 \times 1.25$ โœ“
6 Connected Particles: Pulleys
For particles joined by a light inextensible string over a smooth pulley: the tension is the same on both sides, and both particles have the same magnitude of acceleration. Write an equation for each particle, in its own direction of motion.
5 kg 3 kg T โ†‘ T โ†‘ 5g 3g a โ†“ a โ†‘
Worked Example 7 โ€” Two particles over a pulley

Particles of mass $5$ kg and $3$ kg hang on a light inextensible string over a smooth pulley and are released from rest. Find the acceleration and the tension.

โ‘ $5$ kg (down positive): $5g - T = 5a$.
โ‘ก$3$ kg (up positive): $T - 3g = 3a$.
โ‘ขAdd: $2g = 8a \Rightarrow a = \dfrac{2g}{8} = 2.45$ m s$^{-2}$.
โ‘ฃ$T = 3(g + a) = 3(12.25) = 36.75 \approx 36.8$ N.
The force on the pulley from the string is $2T = 73.5$ N, acting downwards โ€” a common follow-up question.
Worked Example 8 โ€” Table and pulley

A block of mass $4$ kg on a smooth horizontal table is joined by a light inextensible string over a smooth pulley at the table's edge to a particle of mass $1$ kg hanging freely. Find the acceleration and tension.

โ‘ Block (horizontal): $T = 4a$.
โ‘กHanging particle (down positive): $g - T = a$.
โ‘ขAdd: $g = 5a \Rightarrow a = 1.96$ m s$^{-2}$;  $T = 4(1.96) = 7.84$ N.
Do not treat a pulley system as one body with $F = ma$ in a single direction unless you are careful: the weights act in different directions relative to the motion. Writing one equation per particle is always safe.
7 Quick Reference

Newton's 2nd law

Resultant force $= ma$, in the direction of the acceleration.

Weight

$W = mg$, vertically downwards.

Equilibrium

$\sum \mathbf{F} = \mathbf{0}$: at rest or constant velocity.

Vectors

Add $\mathbf{i}$ and $\mathbf{j}$ components separately; $\mathbf{F} = m\mathbf{a}$.

3rd law

Equal and opposite forces on different bodies.

Lift

$R - mg = ma$ (up positive).

Towbar

Tension when pulling; thrust when braking.

Smooth pulley

Same $T$ both sides; same $|a|$; one equation per particle.

Whole system

Internal forces cancel: use it to find $a$ quickly.

8 Practice Questions

Take $g = 9.8$ m s$^{-2}$. Draw a force diagram for every question.

Question 1

A crate of mass $6$ kg is pulled along a horizontal floor by a horizontal force of $40$ N against a resistance of $16$ N. Find its acceleration.

โ–ถ Show solution

$40 - 16 = 6a \Rightarrow a = 4$ m s$^{-2}$.

Question 2

A book of mass $3$ kg rests on a horizontal table. Draw a force diagram and find the normal reaction. State the third-law pair of the normal reaction.

โ–ถ Show solution

Forces on the book: weight $3g$ down, normal reaction $R$ up. Equilibrium: $R = 3g = 29.4$ N.

Its third-law pair is the force of $29.4$ N exerted by the book on the table, acting downwards.

Question 3

Forces $(2\mathbf{i} + \mathbf{j})$ N and $(\mathbf{i} - 5\mathbf{j})$ N act on a particle of mass $0.5$ kg. Find the acceleration and its magnitude.

โ–ถ Show solution

Resultant $= (3\mathbf{i} - 4\mathbf{j})$ N.

$\mathbf{a} = \dfrac{3\mathbf{i} - 4\mathbf{j}}{0.5} = (6\mathbf{i} - 8\mathbf{j})$ m s$^{-2}$;  $|\mathbf{a}| = \sqrt{36 + 64} = 10$ m s$^{-2}$.

Question 4

A particle is in equilibrium under forces $(a\mathbf{i} + 2\mathbf{j})$ N, $(4\mathbf{i} - b\mathbf{j})$ N and $(-7\mathbf{i} + 5\mathbf{j})$ N. Find $a$ and $b$.

โ–ถ Show solution

$\mathbf{i}$: $a + 4 - 7 = 0 \Rightarrow a = 3$.

$\mathbf{j}$: $2 - b + 5 = 0 \Rightarrow b = 7$.

Question 5

A woman of mass $60$ kg stands in a lift that is moving upwards and decelerating at $1.2$ m s$^{-2}$. Find the normal reaction of the floor on her.

โ–ถ Show solution

Up positive; decelerating while moving up means $a = -1.2$.

$R - 60g = 60(-1.2) \Rightarrow R = 588 - 72 = 516$ N.

Question 6

A car of mass $1000$ kg tows a trailer of mass $500$ kg. The car brakes with a braking force of $3000$ N acting on the car only; other resistances are negligible. Find the deceleration and the force in the towbar, stating whether it is a tension or a thrust.

โ–ถ Show solution

Whole system: $-3000 = 1500a \Rightarrow a = -2$, a deceleration of $2$ m s$^{-2}$.

Trailer alone: the only horizontal force is from the towbar, $F = 500(-2) = -1000$ N.

The towbar pushes backwards on the trailer with $1000$ N: it is a thrust.

Question 7

Particles of mass $4$ kg and $6$ kg hang on a light inextensible string over a smooth fixed pulley. Find the acceleration, the tension, and the force exerted on the pulley by the string.

โ–ถ Show solution

$6g - T = 6a$ and $T - 4g = 4a$. Adding: $2g = 10a \Rightarrow a = 1.96$ m s$^{-2}$.

$T = 4(g + a) = 4(11.76) = 47.04 \approx 47.0$ N.

Force on pulley $= 2T = 94.1$ N vertically downwards.

Question 8

A block of mass $3$ kg lies on a rough horizontal table, where a constant resistance of $5$ N opposes its motion. It is connected by a light inextensible string over a smooth pulley at the table's edge to a particle of mass $2$ kg hanging freely. Find the acceleration and the tension.

โ–ถ Show solution

Block: $T - 5 = 3a$.  Hanging particle: $2g - T = 2a$.

Add: $2g - 5 = 5a \Rightarrow 14.6 = 5a \Rightarrow a = 2.92$ m s$^{-2}$.

$T = 2(g - a) = 2(6.88) = 13.76 \approx 13.8$ N. Check: $3(2.92) + 5 = 13.76$ โœ“

Question 9

A particle of mass $2$ kg, initially at rest, is acted on by a constant force $(6\mathbf{i} + 8\mathbf{j})$ N and no other force. Find its speed after $3$ s.

โ–ถ Show solution

$\mathbf{a} = (3\mathbf{i} + 4\mathbf{j})$ m s$^{-2}$, constant.

$\mathbf{v} = \mathbf{u} + \mathbf{a}t = \mathbf{0} + 3(3\mathbf{i} + 4\mathbf{j}) = (9\mathbf{i} + 12\mathbf{j})$ m s$^{-1}$.

Speed $= \sqrt{81 + 144} = 15$ m s$^{-1}$.

Question 10

Particles $A$ (mass $3$ kg) and $B$ (mass $2$ kg) are connected by a light inextensible string over a smooth fixed pulley. They are released from rest with the string taut, $A$ at a height of $1.5$ m above the floor and $B$ well below the pulley.

(a) Find the acceleration and the tension.   (b) Find the speed of $A$ when it hits the floor.   (c) $A$ does not rebound. Find the further distance $B$ rises before coming instantaneously to rest.   (d) State where in your solution you used the fact that the string is inextensible.

โ–ถ Show solution

(a) $A$: $3g - T = 3a$.  $B$: $T - 2g = 2a$. Adding: $g = 5a \Rightarrow a = 1.96$ m s$^{-2}$.

$T = 2(g + a) = 2(11.76) = 23.52 \approx 23.5$ N.

(b) $v^2 = 0 + 2(1.96)(1.5) = 5.88 \Rightarrow v = 2.42$ m s$^{-1}$ (3 s.f.).

(c) When $A$ lands the string goes slack, so $B$ moves freely under gravity with $u = 2.42$ upwards: $0 = 5.88 - 2(9.8)s \Rightarrow s = 0.3$ m.

(d) In (a), taking the same magnitude of acceleration for $A$ and $B$ (and in (b)โ€“(c), the same speed for both when $A$ lands).

Forces and Newton's Laws · A Level Maths Year 1 · Created with MathJax