1 Chapter 4: Forces and Newton’s Laws of Motion Forces Newton’s Three Laws of Motion The...

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1

Chapter 4: Forces and Newton’s Laws of Motion

• Forces• Newton’s Three Laws of Motion• The Gravitational Force• Contact Forces (normal, friction, tension)• Application of Newton’s Second Law• Apparent Weight• Air Resistance• Fundamental Forces• CQ: 16, 18.• P: 3, 5, 21, 37, 41, 63, 73, 87, 97, 147.

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Force Concept

Contact Forces

Ex: car on road, ball bounce

Non-Contact

Ex: magnetism, gravity

/

33

units

• Force units (SI): newton, N

• 1N ≈ ¼ lb.

• 1N = (1kg)(1m/s/s)

• N/kg = m/s/s

s

sm

kg

N /

44

Inertia

• is ‘resistance’ to change in velocity

• Measurement: Mass

• SI Unit: Kilogram (Kg)

• /

55

Universal Law of Gravity

• all matter is weakly attracted

• attraction is inverse-square with distance

• G = 6.67x10-11 N·m2/kg2

• Example: Two 100kg persons stand 1.0m apart

221

r

mmGF

NF 72

11 1067.6)1(

)100)(100(1067.6

66

g vs G

• G is universal

• g ~ Mass and Radius

• /

m

Fg g

2r

MG

mrMm

G 2

mgFw g

7

Contact Forces• Surfaces in contact are often under

compression: each surface pushes against the other. The outward push of each object is called the Normal Force.

• If the objects move (even slightly) parallel to their surface the resistance force experienced is called the frictional force.

88

Normal forces are?

1. Always vertically upward.

2. Always vertically downward.

3. Can point in any direction.

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20

21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40

41 42 43 44 45

9

Tension & Compression

• Compressed objects push outward away from their center (aka Normal Force).

• Stretched objects pull toward their center. This is called the Tension Force.

1010

Force Label Notation

• F = general force

• FN = normal force

• f = frictional force

• w = mg = Fg = weight

• T = tension force

• /

1111

Net Force = change of motion

yxyxamamFF

vector sum of all forces acting on an object

amFnet

xxamF

yyamF

1212

constant velocity

Force Diagram

Fnet = 0

a = 0

Example: Net Force = 0, Ball rolls along a smooth level surface

table force

weight force

13

Example: Net-force on 0.5kg

• Net-force = 4N: Acceleration = 4N/0.5kg = 8m/s/s

• 5N, Right; 3N Left; Net-force = 2NAcceleration = 2N/0.5kg = 4m/s/s

• Falling; Net-force = mgAcceleration = mg/m = g = 9.8m/s/s

• /

1414

1. An object maintains constant velocity when the Net-Force on it is zero.

3. Forces always occur in pairs equal in size and opposite in direction.

2. An object’s acceleration equals the Net-Force on it divided by its mass.

Newton’s Laws of Motion

1515

Force Diagrams

• Object is drawn as a “point”

• Each force is drawn as a “pulling” vector

• Each force is labeled

• Relevant Angles are shown

• x, y axes are written offset from diagram

• Only forces which act ON the object are shown

NF

w F

30

40

1616

Example of a Force Diagram for a Sled

net force equals the mass times its acceleration.

1717

g’s

• one “g” of acceleration = 9.8m/s/s

• “two g’s” = 19.6m/s/s, etc.

• Example: What is the net force on a 2100kg SUV that is accelerating at 0.75g?

• Net-force = ma = m(0.75g) = 0.75mg = ¾ weight of car.

• /

1818

Block on Frictionless Incline

• a = wx/m =mgsin/m

• = gsin.

• Fn = wy.

1919

Newton’s 3rd Law of Motion

• equal-sized oppositely-directed forces

• Independent of mass

• Pair-notation

x x

2020

Newton’s 3rd Law Pair Notation

• use “x” marks on forces that are 3rd Law pairs.

• Use “xx” for a different interaction, etc.

2121

Force Diagram each object. Which has greater acceleration when

released?SpringForce

SpringForce

x x

Acceleration= F/m

Acceleration= F/(2m)

2222

Friction• Static Friction “sticking force”

• Kinetic Friction “sliding force”

• Coefficients: 0 = min, 1 ~ max

• e.g. teflon around 0.05

• Rubber on concretearound 1.0

2323

Using Coefficients of Friction

• Ex. 10kg block. FN = weight = mg = 98N. Static coef. = 0.50; Kinetic coef. = 0.30.

Nss Ff max, Nkk Ff

N

Nf s49

)98)(50.0(max,

N

Nfk29

)98)(30.0(

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Applications

2525

A 3kg object sits on a frictionless table. Two horizontal forces act, one is 2N in the y-direction, the other 4N in the x-direction. A top-view diagram will be shown.

Fnet

What is the magnitude of the net-force acting?

4

22

2,

2, )()(|| ynetxnetnet FFF

490cos20cos4, xnetF

290sin20sin4, ynetF

NFnet 47.4)2()4(|| 22

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What direction does the 3kg mass accelerate?

parallel to Fnet by Newton’s 2nd Law.

),.(180tan,

,1 IIIIIquadsF

F

xnet

ynet

6.26

4

2tan 1

N

N

We are in Quadrant I since x and y are both +

Fnet

4

22

2727

The magnitude of the acceleration is:

ssmkg

N

m

Fa

net//49.1

3

47.4

2828

Two 1kg Blocks; a = 1m/s/s

• Fnet = F = (2m)a = (2kg)(1m/s/s) = 2N

• Fnet = T = ma = (1kg)(1m/s/s) = 1N

• /

F

2929

Two 1kg Blocks; F = 10N

• a = F/(2m) = 10N/2kg = 5 m/s/s

• T = ma = (1kg)(5m/s/s) = 5N

• /

F

3030

4 Summary

• Fnet = ma (Fnet = 0, v = constant)

• forces always occur in pairs of equal size and opposite direction

• various force types (& symbols)

• equilibrium problems (a = 0)

• dynamic problems (a ≠ 0)

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3090

6030

Mg, 300 deg.

32

Inclined Plane Forces

• Fxnet = FNcos90 + mgcos300 = (0.02)(a)

• = 0 + (0.02)(9.8)(0.5) = (0.02)a

• accel = 4.9 m/s/s

• Fynet = FNsin90 + mgsin300 = (0.02)(0)

• FN + (0.02)(9.8)(-.866) = 0

• FN = 0.17N

3333

Fnet

acceleration

Ex: Newton’s 2nd Law

3434

Coefficients of FrictionEx: Block&Load = 580grams

NkgNkgmgFN 68.5)/8.9)(580.0(

If it takes 2.4N to get it moving and 2.0N to keep it moving

42.068.5

4.2max, N

N

F

f

N

ss

35.068.5

0.2

N

N

F

f

N

ks

3535

1. 3kg box on level frictionless surface. F=86N acts 60° below horizontal.

xy

300cos)270cos(90cos)300cos( FwFFF Nx

wFFwFFF NNy 866.0)270sin(90sin)300sin(

NF

F60w

Example:

3636

xy

0xa

0ya

xx maF

2/14

360cos86

60cos

sma

a

maF

x

x

x

yy maF

NF

F

wFF

N

N

N

8.103

)8.9(360sin86

060sin

1.(cont)

3737

Q1. What are ax and FN if angle is 30?NF

F30w

30cos)90cos(90cos)30cos( FwFFF Nx

wFFwFFF NNy 30sin)90sin()30sin(90sin

2/25

330cos86

30cos

sma

a

maF

x

x

x

NF

F

wFF

N

N

N

4.72

)8.9(330sin86

030sin

3838

Interaction Notation

• Since all forces are ‘pairs’, label as interactions, e.g. 1 on 2, 2 on 1, etc.

• F12 = “force of object 1 on object 2”

• F21 = “force of object 2 on object 1”

• F34 = “force of object 3 on object 4”

• Etc.

3939

Interaction Notation Symbols

• F12 – general force, 1 on 2

• N12 – normal contact force, 1 on 2

• f12 – frictional force, 1 on 2

• W12 – gravitational force, 1 on 2

• T12 – tension force, 1 on 2

• m12 – magnetic force, 1 on 2

• e12 – electrical force, 1 on 2

4040

Gravitational Force

• All masses attract via gravitational force

• Attraction is weak for two small objects

• Ex: Attraction between two bowling balls is so small it is hard to measure.

• Force is proportional to mass product

• Force is inversely proportional to the square of the distance between objects

4141

Example: Net Force = 0. Block on a surface inclined 30° from horizontal. Applied force F acts 40° below horizontal.

NF

w F

30

40

Net Force = 0

velocity = constant

4242

Diagrams with Interaction Notation

• If f21 exists, then f12 also exists, and is opposite in direction to f21.

• f21 and f12 act on different objects.

4343

A 10kg box is being pushed along a horizontal surface by a force of 15N. A frictional force of 5N acts against the motion. We will want to (a) Calculate the net-force acting and (b) calculate the acceleration of the box.

xx maNNNF 10515

0. yy maweightforceNormalF

The net-horizontal force determines its x-acceleration

The y-acceleration is known to be zero because it remains in horizontal motion, thus

The net-force is 10N horizontal (0 vertical)

The x-acceleration is: ssmkg

N

m

Fa xx //1

10

10

Example: