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Forces and Newtons Laws of Motion Module 1: Mechanics
73

Kragte 11 e

Aug 10, 2015

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Page 1: Kragte 11 e

Forces and

Newtons Laws of Motion

Module 1: Mechanics

Page 2: Kragte 11 e

Introduction to forces

A force is a pull or a push that an object experiences due to its interaction with other objects.

Definition

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Properties Symbol: SI-unit: Vector

๐‘ญแˆฌแˆฌิฆ Newton (N)

Introduction to forces

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Types of ForcesContact Forces

Non-contact Forces

Forces that are exerted by

objects that make contact

with each other

Forces exerted by objects that do NOT make

contact with each other

Introduction to forces

Page 5: Kragte 11 e

Contact Forces Applied Force ():

A force is exerted on an object by someone

Introduction to forces

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Tension ():- A force exerted by a rope or cable when it is pulled.

- The same everywhere in the rope/cable.

Contact ForcesIntroduction to forces

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Friction ():- A force between and object and the

surface on which it rests parallel to the surface.

- Always opposes motion

๐’—แˆฌแˆฌิฆ ๏ฟฝโƒ—๏ฟฝ

Contact ForcesIntroduction to forces

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Normal force ():- The force that a surface exerts on the

object that rests on it.- Always perpendicular from the surface

on the object.

Contact ForcesIntroduction to forces

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Weight ():- The force with which the earth

attracts an object- Always downwards-

where

Contact ForcesIntroduction to forces

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Magnetic Force ():- The force that magnets exert on

other ferromagnetic objects.- Repulsive or Attractive

Non-contact ForcesIntroduction to forces

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Electrostatic Force ():- The force that charged objects

exert on other objects- Repulsive or Attractive

Non-contact ForcesIntroduction to forces

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Example 1Identify all the forces present in the following pictures:

On the trolley

a) On the balloon

b) On the basket

Introduction to forces

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Representation of ForcesForce Diagrams

The object itself is represented diagramatically

Forces are shown with arrows where it really works on the object.

Lengths of the arrows shows the relative magnitudes of the forces

Page 14: Kragte 11 e

Representation of ForcesExample 2

Draw a force diagram that shows all the forces that are exerted on the trolley

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ

๐‘ญ๐‘ท๐’๐’‚๐’๐’•๐’†แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ป๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ป๐’šแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Page 15: Kragte 11 e

Freebody diagrams FREE OF A BODY Object represented by only a dot All arrows must point from the dot

outwards Lengths of the arrows shows the

relative magnitudes of the forces

Representation of Forces

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Example 3Draw a free body diagram that shows all the forces exerted on the trolley๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ ๐‘ญ๐‘ท๐’๐’‚๐’๐’•๐’†แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ป๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ป๐’šแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Representation of Forces

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Triangle of ForcesForces in equilibrium

All the forces exerted on a certain point cancel each other

The resultant of the forces are zero The object remains in rest or moves

with a constant velocity When all the forces are drawn head

to tail it forms a CLOSED vector diagram.

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Example

NO RESULTANT

Triangle of Forces

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When three forces that are exerted on the same point

are in equilibrium, their magnitudes and direction can be shown by the three

sides of a triangle.

Triangle of Forces

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FrictionTypes of Friction

Static Friction Kinetic Friction

Exerted on

Symbol

Properties

Formula

Objects in rest Moving Objects

Changes as the applied force

changesAlways constant

๐’‡๐’Œแˆฌแˆฌแˆฌแˆฌิฆ ๐’‡๐’”แˆฌแˆฌแˆฌแˆฌิฆ

๐’‡๐’Œแˆฌแˆฌแˆฌแˆฌิฆ= ๐๐’Œ๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐’‡๐’” ๐’Ž๐’‚๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐๐’”๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Page 21: Kragte 11 e

WrywingTipes wrywing๐’‡๐’”แˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ

๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡๐’Œแˆฌแˆฌแˆฌแˆฌิฆ

๐’—แˆฌแˆฌิฆ= ๐ŸŽ ๐’—แˆฌแˆฌิฆ> ๐ŸŽ

๐’‡๐’”แˆฌแˆฌแˆฌแˆฌิฆ ๐’‡๐’Œแˆฌแˆฌแˆฌแˆฌิฆ ๐’‡๐’” ๐’Ž๐’‚๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

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FrictionMaximum Static Friction

The static friction that an object experiences just before it moves. Static friction increases as the force it opposes increases, until it reaches a maximum. If the applied force increases further, the object starts to move. The object now experiences kinetic friction.

Page 23: Kragte 11 e

Friction

๐’‡แˆฌิฆ= ๐๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Friction

Static/kinetic Coeficient of Friction

Normal Force

Formula

Page 24: Kragte 11 e

FrictionProperties

Strongly dependent on surface roughness. Directly proportional to the normal force. Indipendent on the surface area of the surfaces in contact. Kinetic friction is independent of the speed at which the object moves. Only the maximum static friction can be calculated with a formula ๐’‡๐’Œแˆฌแˆฌแˆฌแˆฌิฆ< ๐’‡๐’” ๐’Ž๐’‚๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Page 25: Kragte 11 e

FrictionCoefisient of Friction

ฮผ No unit Property of the surfaces in contact Mostly smaller than one The bigger ฮผ, the bigger the friction ๐œ‡๐‘˜ < ๐œ‡๐‘ 

Page 26: Kragte 11 e

Net force of two or more forces

The net force of all the forces that are exerted on an object, is the vector sum of all the

forces that are exerted on the object.

Page 27: Kragte 11 e

Also known as the resultant force The net forces in the x-axis an

y-axis are calculated separately

Inclined forces are separated into perpendicular components.

๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ต๐‘ฌ๐‘ป ๐’™แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญ๐’™แˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ต๐‘ฌ๐‘ป ๐’šแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญ๐’šแˆฌแˆฌแˆฌแˆฌิฆ

Net force of two or more forces

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Net ForceExample 1

A book is pulled over a rough surface with a constant force. The kinetic friction coefficient between the surface and the book is 0,5. All the forces are in equilibrium.a) Draw a free body diagramb) Determine the normal forcec) Calculate the kinetic frictiond) Calculate the applied force

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Net forceExample 2

The same book as in the previous example is now being pulled across the table by an 5 N force, that makes an angle of 30ยฐ with the horizontal. a) Calculate the kinetic friction.b) How does the value of the friction

compare to the value in the previous exmaple? Explain.

c) Calculate the net force in the x-axis

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Forces on an incline plane

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ฮธ

๐’‡แˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

โˆฅโŠฅ

Page 31: Kragte 11 e

Forces on an inclined plane

ฮธฮธ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐’ˆโŠฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐’ˆโˆฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐’”๐’Š๐’๐œฝ= ๐‘ญ๐’ˆโˆฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐’ˆโˆฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ๐’”๐’Š๐’๐œฝ

๐‘ญ๐’ˆโŠฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ๐’„๐’๐’”๐œฝ

๐’„๐’๐’”๐œฝ= ๐‘ญ๐’ˆโŠฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

90ยฐ

โˆฅโŠฅ

Page 32: Kragte 11 e

Net ForceExample 3

All the forces exerted on the crate in the diagram are in equilibrium. Answer the following questions:a) Draw a free body diagram.b) Calculate and . c) Calculate the normal force.d) Calculate the kinetic friction.e) Calculate

๐‘ญ๐’ˆโˆฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐’ˆโŠฅแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐๐’Œ

Page 33: Kragte 11 e

Net forceExample 3

5 kg

25ยฐ

Page 34: Kragte 11 e

Newtonโ€™s Laws of Motion

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Eureka!!!

Father of Mechanics, modern Calculus,

Astronomy and Optics

Sir Isaac Newton

1642-1727

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Newton IIIAction-Reaction

If object A exerts a force on object B, object B will exert a force on object A that has the same magnitude, but opposite

direction.

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Newton IIIAction-Reaction

A B

A:

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ

๐‘ญ๐‘ฉ๐‘จแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐’‡แˆฌิฆ

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘จ๐‘ฉแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

B:

๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

Page 39: Kragte 11 e

Newton IIIForce pairs

but opposite in direction Is NOT exerted on the same object Do NOT cancel eachother Works SIMULTANEOUSLY

- THEREFORE: For each action there is a reaction

๐‘ญ๐‘จ๐‘ฉแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญ๐‘ฉ๐‘จแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Page 40: Kragte 11 e

Newton IIIExample

Identify the Newton III force pairs in the following diagram.

Page 41: Kragte 11 e

A:

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ

๐‘ญ๐‘ฉ๐‘จแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐‘ญ๐‘ปแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ ๐’‡แˆฌิฆ

๐‘ญ๐’ˆแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐‘ญ๐‘จ๐‘ฉแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

B:

Newton IIIForce pairs

Newton III Force Pairs

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Newton ILaw of Inertia

An object will remain in a state of rest, or move with a constant

velocity in a straight line, unless a net force is exerted on the object.

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Newton ILaw of Innertia

In Symbols:๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐ŸŽ ๐‘ต

if

๐’—แˆฌแˆฌิฆ= ๐ŸŽ ๐’Žโˆ™๐’”โˆ’๐Ÿ โˆด ๐’‚แˆฌแˆฌิฆ= ๐ŸŽ ๐’Žโˆ™๐’”โˆ’๐Ÿ

๏ฟฝโƒ—๏ฟฝ=๐’„๐’๐’๐’”๐’•๐’‚๐’๐’•

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Newton IInertia

The property of an object that causes it to resist a change in its

state of motion

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Newton IInnertia

A property of the object All objects with mass have innertia Bigger mass = More innertia

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Newton IIForce and AccelerationIf a net force is exerted on an

object, the object will accelerate in the direction of the force. The

acceleration is directly proportional to the force and inversely

proportional to the mass of the object.

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Newton IIForce and Acceleration

In Symbols:๐‘ญ๐‘ต๐’†๐’•แˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐’Ž๐’‚แˆฌแˆฌิฆ

where ๏ฟฝโƒ—๏ฟฝ ๐‘ต๐‘ฌ๐‘ป=๐‘ต๐’†๐’•๐‘ญ๐’๐’“๐’„๐’† (๐‘ต)๐’Ž=๐’Ž๐’‚๐’”๐’” (๐’Œ๐’ˆ)๐’‚=๐’‚๐’„๐’„๐’†๐’๐’†๐’“๐’‚๐’•๐’Š๐’๐’ (๐’Žโˆ™ ๐’”โˆ’๐Ÿ)

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Newton IIForce and Acceleration๐’‚แˆฌแˆฌิฆโˆ ๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Direct proportionality =

Straight line through origin

๐’‚แˆฌแˆฌิฆ

๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

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Newton II

๐’‚แˆฌแˆฌิฆโˆ ๐Ÿ๐’Ž

Inverse proportionality =

Hyperbole

๐’‚แˆฌแˆฌิฆ

๐’Ž

Force and Acceleration

Page 50: Kragte 11 e

๐’‚แˆฌแˆฌิฆ

๐Ÿ๐’Ž

Newton II

๐’‚แˆฌแˆฌิฆโˆ ๐Ÿ๐’Ž

Straight line

Force and Acceleration

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Newtonโ€™s LawsSolving of Problems

1) Separate inclined forces into perpendicular components

2) Draw free body diagrams3) Identify the applicable axis.

Handle the x-axis and y-axis separately.

4) Obtain an equation for๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Page 52: Kragte 11 e

๐’—แˆฌแˆฌิฆ= ๐ŸŽ ๐’Žโˆ™๐’”โˆ’๐Ÿ

Newton I Newton II

๐’‚แˆฌแˆฌิฆโ‰  ๐ŸŽ ๐’Žโˆ™๐’”โˆ’๐Ÿ

5) Decide which law you will use:

๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐ŸŽ ๐ ๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐’Ž๐’‚แˆฌแˆฌิฆ

Newtonโ€™s LawsSolving of Problems

๏ฟฝโƒ—๏ฟฝ=๐’„๐’๐’๐’”๐’•๐’‚๐’๐’•

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6) Check for friction:ฮผ is given

YES NO

Calculate with:๐‘ญ๐‘ต๐‘ฌ๐‘ปแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌแˆฌิฆ= ๐‘ญแˆฌแˆฌิฆ

Calculate ๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

Calculate with:๐’‡แˆฌิฆ ๐’‡แˆฌิฆ= ๐๐‘ญ๐‘ตแˆฌแˆฌแˆฌแˆฌแˆฌิฆ

๐’‡แˆฌิฆ

Newtonโ€™s LawsSolving of Problems

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Example 1A Block, mass 5 kg, is being pulled across a horizontal table with a constant force of 50 N. The magnitude of the friction is, 20 N. Calculate:a) The acceleration of the block.b) The friction coefficient between the

block and the table.

Newtonโ€™s Laws

Page 55: Kragte 11 e

A boy pushes a crate of 50 kg over the floor with the aid of a rod that makes an angle of 40ยฐ with the horizontal. He exerts a force of 300 N on the rod. The friction coefficient between the crate and the floor is 0,2.

Newtonโ€™s Laws

Example 2

Page 56: Kragte 11 e

a) Calculate the friction between the floor and the crate.

b) Calculate the acceleration of the crate.

300 N

40ยฐ

Example 2Newtonโ€™s Laws

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A person skiโ€™s down a slope that makes an angle of 40ยฐ with the horizontal. The total mass of the skier and his skiโ€™s is 50 kg. The friction coefficient between the snow and the skiโ€™s are 0,1.a) Calculate the net force the person

experience parallel to the surface.b) Calculate the acceleration of the skier.

Example 3Newtonโ€™s Laws

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The diagram shows a 3 kg block (B) and a 2 kg block (A) that is being pushed forward by a force of 30 N so that the system accelerates to the right. The applied force makes an angle of 15ยฐ with the horizontal. Each block experiences a friction force of 5 N.

Example 4Newtonโ€™s Laws

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15ยฐ

a) Calculate the acceleration of the system.

b) Calculate the force that A exerts on B.c) Calculate the force that B exerts on A.

A B

Example 4Newtonโ€™s Laws

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B

6 kg

A4 kg

C6 kg

T1 T2

Example 5Newtonโ€™s Laws

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The friction coefficient between Block B and the table top is 0,034. Assume that the ropes have negligible mass and that the pulleys are frictionless. Calculate:a) The acceleration of the system.b) The tension in the ropes..

Example 5Newtonโ€™s Laws

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A man with a mass of 70 kg stands on a scale in a lift. Calculate the reading on the scale if the lift:a) Is in rest.b) Moves upward with a constant velocity

of 3,2 mยทs-1.c) Accelerates upward at 3,2 mยทs-2.d) Accelerates downward at 3,2 mยทs-2.e) Freefall

Example 6Newtonโ€™s Laws

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Universal Gravitation

Between any two objects with mass there exist a gravitation force that is directly proportional to the product of

their masses and inversely proportional to the square of the

distance between their centre points.

Newtonโ€™s Laws

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Universal GravitationSymbols

๏ฟฝโƒ—๏ฟฝ๐‘ฎ=๐‘ฎ๐’Ž๐Ÿ๐’Ž๐Ÿ

๐’“๐Ÿ

๐’“๐’Ž๐Ÿ ๐’Ž๐Ÿ

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Universal GravitationSymbols

= Gravitation force (N) = Mass of objects (kg) = Distance between objects (m) = Universal Gravitation

Constant= 6,67 x 10-11 Nยทm2ยทkg-2

๏ฟฝโƒ—๏ฟฝ๐‘ฎ=๐‘ฎ๐’Ž๐Ÿ๐’Ž๐Ÿ

๐’“๐Ÿ

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Universal GravitationSymbols: On a Planet

๏ฟฝโƒ—๏ฟฝ๐‘ฎ=๐‘ฎ๐’Ž๐‘ด๐‘น๐Ÿ

= Massa van planeet (kg) = Massa van vorrwerp

(kg) = Radius van planeet (m)

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Universal GravitationRelationship between G and g

๏ฟฝโƒ—๏ฟฝ๐‘ฎ=๐‘ฎ๐’Ž๐‘ด๐‘น๐Ÿ

Attraction force by earth on object:

๏ฟฝโƒ—๏ฟฝ๐’ˆ=๐’Ž๐’ˆand

๏ฟฝโƒ—๏ฟฝ๐‘ฎ= ๏ฟฝโƒ—๏ฟฝ๐’ˆbut

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๐‘ฎ๐’Ž๐‘ด๐‘น๐Ÿ =๐’Ž๐’ˆ

Universal Gravitation

therefore รท๐’Ž

๐’ˆ=๐‘ฎ๐‘ด๐‘น๐Ÿ

Relationship between G and g

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Amount of matter Symbol: m Unit: kg Scalar The same everywhere

Universal GravitationMass

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Universele GravitasieGewig

Force with which planets attract an object

Symbol: Unit: N Vector Function of the mass and

radius of a planet

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Universal GravitationExample 1

Two spherical objects m1 and m2, with their centre points a distance r metre apart, exerts a gravitation force of 6 N on each other. Determine the magnitude of the force if:a) The mass m1 doubles.b) The distance between them halves.

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Universal GravitationExample 2

Two metal spheres with masses 8 x 104 kg and 2 x 103 kg respectively is placed 340 cm apart. Calculate the gravitation force between them.

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Universal GravitationExample 3

An astronaut with a mass of 80 kg on the earth lands on planet X with his spaceship. Planet X has a radius that is half that of the earth ant a mass that is double that of the earth.

a) Calculate the value of g on planet X.b) Calculate the garvitation force that the

man experiences on planet X.