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Topic 7 Gra-vi-ta-tion-al Field by mr jimmy goh

Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

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Page 1: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

Topic 7

Gra-vi-ta-tion-al Field

by mr jimmy goh

Page 2: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

What do you know about the

Gravitational field?

Gravity?

Weight?

9.81?

Pull things downward?

Make things feel heavy?

Page 3: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

Overview of this topic

1. Newton’s Law of Gravitation

2. Gravitation field & Gravitational field

strength

3. Gravitational potential energy & potential

4. Satellites in orbit

Page 4: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

Learning outcomes

2. Field strength (vector)

1. Newton’s law of Gravitation

Page 5: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

Learning outcomes 3. Potential (scalar)

4. Satellite in orbit

Page 6: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.1 Introduction

Guess my weight.

What is the unit of weight?

What is weight?

A force due to gravitational field of Earth

What affects its magnitude?

The mass of the object

The value of g (also known as acceleration due to gravity)

Page 7: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.1 Introduction

What do you know about Earth?

Oblate spheroid: a sphere flattened along the axis from

pole to pole such that there is a bulge around the equator.

Average radius of

Earth is 6400 km

North pole

South pole

Equator

Diameter at the

equator is 43 km

longer than the pole

to pole diameter

Axis of

rotation

SUN E W

Rotates about its

pole to pole axis

Rotates from

West to East

Page 8: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.1 Introduction

Earth is a rocky planet with a huge mass of 6.0 x 1024 kg.

Because of its mass, it has a strong gravitational field

around it that attracts everything that has mass towards

itself.

What happens when you drop an apple in air?

It will fall down.

It will accelerate

towards the centre

of the Earth.

Page 9: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.1 Introduction

Earth is not the only planet that can attract other masses.

Ocean tides are caused by the

gravitational attraction of the Moon

on the earth’s oceans

Gravitational force is responsible for

keeping the Earth in its orbit around

the Sun.

Page 10: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation

Page 11: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation Not radius!

Page 12: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation

Page 13: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation

Page 14: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation

3.8 108 m

x

Net gravitational field

strength & potential by

Earth & Moon Model

FCE FCM

Page 15: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.2 Newton’s law of Gravitation

FCE FCM

Square

root both

sides

Page 16: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.3 Gravitational Field

Do you have

gravitational field?

Page 17: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.3 Gravitational Field

The gravitational field near

Earth’s surface is uniform

The closer the field lines, the

stronger the field strength.

The field lines should be

drawn parallel to each other

and of equal spacing.

These are called the field lines.

Page 18: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.3 Gravitational Field

The gravitational field around Earth is

non-uniform.

The field lines should be drawn radially

pointing towards the centre of Earth.

The field lines get further apart (field

strength decreases) as it gets further

from Earth.

Page 19: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.3 Gravitational Field

Page 20: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

20 N

For example, if a 5 kg point mass is placed at distance r1 away from Earth and it

experiences a gravitational force of 20 N, calculate the gravitational field strength

at r1.

5 kg

r1

At r1, g = 20 N / 5 kg = 4 N kg-1 or 4 m s-2

Also known as the

acceleration due to gravity

r1

5 kg 20 N 5 N

r2

5 kg

At r2, g = 5 N / 5 kg = 1 N kg-1 or 1 m s-2

What happen if

a 100 kg is

placed at r2?

Page 21: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

20 N

For example, if a 5 kg point mass is placed at distance r1 away from Earth and it

experiences a gravitational force of 20 N, calculate the gravitational field strength

at r1.

5 kg

r1

At r1, g = 20 N / 5 kg = 4 N kg-1 or 4 m s-2

Also known as the

acceleration due to gravity

r1

5 kg 20 N 100 N

r2

100 kg

At r2, g = 5 N / 5 kg = 1 N kg-1 or 1 m s-2

What happen if

a 100 kg is

placed at r2?

Field strength gives a

clearer indication..

Page 22: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

4 N kg-1

For example, if a 5 kg point mass is placed at distance r1 away from Earth and it

experiences a gravitational force of 20 N, calculate the gravitational field strength

at r1.

r1

At r1, g = 20 N / 5 kg = 4 N kg-1 or 4 m s-2

Also known as the

acceleration due to gravity

r1

r2

At r2, g = 5 N / 5 kg = 1 N kg-1 or 1 m s-2

4 N kg-1 1 N kg-1

Page 23: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

F

F1

F2

F3

Page 24: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

Source mass

Page 25: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

Gravitational field

strength &

potential Model

Page 26: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

g1 g2 g3

g4

Page 27: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

Page 28: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

gE gM

Page 29: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

gE gM

Page 30: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.4 Gravitational Field Strength

Page 31: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.5 Gravitational Potential Energy

In topic 5 (Work Energy Power), G.P.E. = mgh

5 kg

10 m

G.P.E. = mgh

= (5) (9.81) (10)

= 491 J

15 m

Reference = 0 m

Reference = 0 m

G.P.E. = mgh

= (5) (9.81) (15)

= 736 J

Which is the actual G.P.E. of the 5 kg object?

Therefore, mgh does not give

us the actual G.P.E. of object.

Instead, mgh indicates the

change in G.P.E. of object.

Furthermore, the g value

(9.81) is only for short

heights from Earth surface.

Page 32: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.5 Gravitational Potential Energy

Infinity

U = 0 J

(max) r

M

m As r increases

U = - 100 J U = - 50 J

U increases

Page 33: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.5 Gravitational Potential Energy

r

s Fext

That point Gravitational field

strength &

potential Model

Page 34: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.5 Gravitational Potential Energy

r

s Fext

That point

Because F and s

are in opposite

direction!

Page 35: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.5 Gravitational Potential Energy

Page 36: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.6 Gravitational Potential

Page 37: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.6 Gravitational Potential

Page 38: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.6 Gravitational Potential

gA gB

gC

Page 39: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.6 Gravitational Potential

gA gB

gC

Page 40: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

Compare & Contrast

-ve sign:

pointing in –ve

direction -ve sign: less

than zero

Page 41: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.7 Relationship between F & U

Page 42: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.7 Relationship between g & ɸ

Page 43: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.7 Relationship between g & ɸ

Page 44: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.7 Relationship between g & ɸ

r /m

ɸ /MJ kg-1

-62.72

- 59.12

- 59.03

- 58.94

400 000

Page 45: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.8 Satellite in orbit Launching a

satellite video

Page 46: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.8 Satellite in orbit

Page 47: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.8 Satellite in orbit

Page 48: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.9 Kepler’s Third Law

Kepler’s 3rd Law

Model

What can this tell us about

the rotation of different

planets around the Sun?

What happen to the

period of rotation if the

mass of satellite is

increased?

Page 49: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Geostationary

Orbit Model

North pole

South pole

Equator

E W

Page 50: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Axis of rotation

Page 51: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Page 52: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Page 53: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Page 54: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.10 Geostationary Satellites

Since V = r ω = r ( 2π / T),

Page 55: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.11 Energy of a Satellite in orbit

Page 56: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.11 Energy of a Satellite in orbit

2

2

Only for satellite in orbit!

Page 57: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.11 Energy of a Satellite in orbit

EK = − ET

EP = 2 ET

Page 58: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.11 Energy of a Satellite in orbit Add in: Mass of Earth = 6.0 x 1024 kg

Page 59: Gravitational Field Lectures by Mr Jimmy Goh (for LMS)

7.11 Energy of a Satellite in orbit Mass of Earth = 6.0 x 1024 kg