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Dr Chris Skilbeck Newton’s Laws of Motion An Introduction to Mechanics
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Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

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Page 1: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Dr Chris Skilbeck

Newton’s Laws of Motion

An Introduction to Mechanics

Page 2: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Topics Covered:

1. Newton’s Laws of Motion

2. Force Diagrams

3. Introduction to Calculus and vectors

Page 3: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

The Laws of Motion

Aristotle (384-322 BC)1. The natural state of motion is

rest

2. Where there is motion, it must be caused by an external agent or force that overcomes the natural reluctance of objects to move

Why are these laws incorrect?!

Page 4: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

The Laws of MotionIsaac Newton (1642 – 1727)1. The natural state of motion is

uniform progress along a straight line – motion is constant at constant velocity and zero acceleration in the absence of forces

2. Acceleration is caused by external forces

Page 5: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Newton’s Laws of Motion

1. An object either moves in a straight line at constant velocity or remains at rest if no external force acts upon it

2. Force = mass x acceleration: F = ma

Force and acceleration are vector quantities, mass is a scalar quantity

3. For every force there is an equal and opposite reaction

Page 6: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

F = ma a = F/mx-axis

Motion in One Dimension

m = 50 g, a = 9.81 m/s2

a is acceleration due to gravity

Q.1 What is F?

Page 7: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Vectors

• Force and acceleration are vectors

• They have both magnitude and direction

• Can be represented in diagrams by arrows

• Length of arrow = magnitude

• Vectors written as: a or a or ā

• Magnitude of a = |a| = a

• Vectors have components, e.g. F = Fx + Fy + Fz

kFjFiFF zyxˆˆˆ

Page 8: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

kji ˆ,ˆ,ˆ Are unit vectors: point in positive x, y and z-axis directions, but have magnitude = 1

z

x

y

Coordinate Systems

ij

k

Left or Right-handed coordinates?

Page 9: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Resolving Vectors

y

x

r (7,5)

What are the lengths of the components of the vector r, which lies in the y and x-directions (ryand rx respectively)?

Hint: SOHCAHTOA

Page 10: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Radians

Circle: radius r

circumference = 2r

area = r2

360o or 2 rad

r

r arc length, L

L = r

with in rad

1 rad ≈ 57o 17' 45''

When L = r:

= 1 rad

So: 1 rad is the angle of the sector when L = r

Area of sector: A = ½r2

o180radiansin angle degreesin Angle

Page 11: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Q.2 How many radians is 180o?

Q.3 How many degrees is 2/ rad?

Q.4 how many radians is 120 degrees?

Page 12: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Motion in One Dimension

• We can simplify by choosing the x-axis to be parallel to direction of motion

• Vector equations reduce to scalar equations: a force acting towards +x is positive, a force acting towards –x is negative

Page 13: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

F = ma a = F/mx-axis

Motion in One Dimension

m = 50 g, a = 9.81 m/s2

a is acceleration due to gravity

Q.1 What is F?

Page 14: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Constant Acceleration in One Dimension

• Close to the surface of the Earth the force of gravity is approximately constant = 9.81 m/s2 at surface of earth

• Acceleration due to gravity is approximately constant: a = c

vx

t

vx = at + ux

ax

t

ax = 9.81 m/s2

9.81

Uniformly accelerated motion

uxQ. 5 What is ux?

Page 15: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Practice Questions

Q. 6

A sky-jumper is in free-fall. What is their velocity after 10 seconds? [g = 9.81 m/s2; assume there is no air resistance.]

Q.7

In practice, the terminal ‘velocity’ of a skydiver is about 55 m/s. Why is this?

Page 16: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus

• Calculus studies rates of change / how one variable changes as another changes, e.g. how velocity changes over time

Acceleration = change in velocity / change in time

tva

This is the gradient of the velocity-time curve!

Acceleration is a function of time: a = a(t)

Page 17: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus

Q

txv

Velocity = change in distance / change in time

This is the gradient of the distance-time curve!

x

t

distance, x

time, t

x + x

x

t + tt0

How do we get the gradient at point

Q = (x + ½x, t + ½t)

?

Page 18: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Qx

t

distance, x(t)

time, t

x(t + t)

x(t)

t + tt0

Introduction to Calculus

1D motion: distance moved along the x-axis is a function of time: x = x(t)

gradient =x(t + t) – x(t)

t + t - t

x(t + t) – x(t)

t=

Page 19: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Qx

t

distance, x(t)

time, t

x(t + t)

x(t)

t + tt0

Introduction to Calculus

1D motion: distance moved along the x-axis is a function of time: x = x(t)

gradient at Q =x(t + t) – x(t)

tlim

t → 0

x

tlim

t → 0=

=dtdx

Page 20: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - Limits

• Mathematics is not always intuitive!

• What is the sum of the following series for an infinite number of terms?

18 + 1.8 +0.18 +0.018 +0.0018 + 0.00018 + …

S2 = 19.8

S3 = 19.98

S4 = 19.998

S5 = 19.9998

S6 = 19.99998

S7 = 19.999998

For an infinite number of terms the sum S∞ = 20

As we can never count to infinity we say: Sn → ∞ as n →∞

or lim Sn = 20

The limit of Sn tends to 20 as n tends to infinity

n→∞

Page 21: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - Differentiation

• Differentiation gives us the gradient of a curve at a point

• This is immensely useful !!!!!

From the distance-time graph, the velocity at any instant of time is the gradient at time t:

v = dx / dt

From the velocity-time graph, the acceleration at any instant of time is the gradient at time t:

a = dv / dt

Page 22: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - Differentiation

For a function f(t), the derivative of f with respects to t, df/dt:

f(t) = c = constant df/dt = 0 why?

f(t) = t df/dt = 1 why?

f(t) = 2t df/dt = 2 why?

f(t) = t2 df/dt = 2t

General:

f(t) = htn + g df/dt = nhtn-1

Page 23: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - Differentiation

For y = y(x), where a, b = constant

acos(ax)sin(ax)

-asin(ax)cos(ax)

aeaxeax = exp(ax)

1/x (for ax > 0)ln(ax) = loge(ax)

abxa-1bxa

axa-1xa

0a

derivative dy/dxFunction y(x)

Page 24: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

• v = v(t) for motion along the x-axis we can use scalar quantities, velocity is a vector, speed is a scalar, so: v = v(t)

• a = a(t)

• v = dx/dt

• a = dv/dt

For uniformly accelerated motion:

|a| = c = constant

How do we obtain v and x ?

Introduction to Calculus - Differentiation

Page 25: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Q.8 A particle of mass 2 kg oscillates along the x-axis according to the equation:

65sin2.0 tx

Where x is in m, t in s.

(a)What is the force acting on the particle at t = 0?

(b)What is the maximum force that acts on the particle?

Page 26: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - Integration

• Integration is the reverse of differentiation!

• Differentiation gives us the gradient of a curve

• Integration gives us the area under a curve

• dx/dt is the derivative of x with respects to t

• ∫x(t)dt is the integral of x with respects to t

Page 27: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

y

x

y = x

dy/dx = 1

The gradient = 1 for all points along the line!

Area under the curve

dy/dx of (y = xa) = axa-1

aa xdxax 1

21

21 xdxxxdx

11 aa xa

dxx

1 aa axxdxd

aa xxadx

d11

Introduction to Calculus - Integration

Area of a triangle?

Page 28: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Introduction to Calculus - IntegrationFor y = y(x), where a, b = constant

cos(ax)

sin(ax)

eax

xa for a ≠ -1axa

a = constant0

integral ∫y(x)dxFunction y(x)

1

1

axa

axea1

)cos(1 axa

)sin(1 axa

Page 29: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Equations of Motion

For uniformly accelerated motion in one direction: adtdv

Integrate w.r.t. t to get v: catv

What is the constant C? It is the initial velocity, u (or v0), of the object at time t = 0, when v = u, so:

uatv

Integrate w.r.t. t to get distance moved, s:

utats 2

21

Page 30: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Equations of Motion – Constant Acceleration Equations

Uniformly accelerated motion along x-axis: a = constant

constant xx a

dtdv

xxx utav

tutas xxx 2

21

Fx = max

Page 31: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Uniform Motion and Newton’s First Law

An object either moves in a straight line at constant velocity or remains at rest if no external force acts upon it

Uniform motion: No force acts on the object, its acceleration is zero

In 1D:

ax = 0

vx = ux

sx = uxt

The uniform motion equations

Page 32: Newton’s Laws of Motion An Introduction to Mechanics · Newton’s Laws of Motion 1.An object either moves in a straight line at constant velocity or remains at rest if no external

Practice Questions

Q.9

A spaceship is drifting in space, moving in a straight line with speed 12 km/s. How far will it have drifted: a) in 1 hour, b) in one year? [Assume negligible ‘air’resistance.]

Q.10

A man drops from a 30 metre balcony. Assuming he was initially stationary, how long will it take him to reach the ground? What will be his speed on impact? [g = 9.81 m/s2].