Forces, Acceleration & Newton's Laws: Understanding the Relationship, Summaries of Physics

An in-depth exploration of the relationship between forces and acceleration, focusing on vector addition and Newton's second and third laws. Students will learn how to calculate the sum of forces acting on an object and understand the significance of Newton's laws in various scenarios. examples and exercises to help solidify the concepts.

Typology: Summaries

2021/2022

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This Week
Textbook -- Read Cha pter 4, 5
Competent Problem Solver - Chapter 4
Pre-lab Computer Qui z
What’s on the next Quiz?
Kinematics - Everythi ng
Forces - to lectur e before quiz
Check Your Understanding at
end of each Labora tory is a
good guide
Work problems as if ta king the quiz:
Assigned homework - minimum
if you can do them easily
Problems at end of cha pter 3 and 4
of CPS
Check out sample quiz on web by Thurs.
Other textbook problems
What you missed on first quiz
The combined effect of ALL forces on an
object that determines i ts acceleration.
The effects of forces in perpendicular
directions are inde pendent
Forces are vector qua ntities
Combining Forces me ans Vector Addition
Theory of Forces
The Mathematics:
Define a coordinate system
with perpendicular x and y axes
Add x components of forces
and independentl y
Add y components of forces
+y
+x
F
1
F
2
Example: 2 forces act on an object, how
does it move?
+y
+x
F
1
F
2
Adding Forces
Σ
Σ Σ
Σ F = F
1
+ F
2
means
Σ
Σ Σ
Σ F
x
= F
1x
+ F
2x
and
Σ
Σ Σ
Σ F
y
= F
1y
+ F
2y
F
1x
F
2x
+y
+x
Σ
ΣΣ
ΣF
x
=F
1x
+ F
2x
F
1y
F
2y
Σ
ΣΣ
ΣF
y
=F
1y
+ F
2y
Σ
ΣΣ
ΣF
θ
θθ
θ
F
=
==
=F
x
(
((
()
))
)
2
+
++
+F
y
(
((
()
))
)
2
tanθ
θθ
θ=
==
=F
y
F
x
First: Take the vectors apart
Second: Put the resulting vector together
The sum of the xcomponents of Forces
Σ
ΣΣ
ΣF
x
the xcomponent of acceleration
The sum of the ycomponents of Forces
Σ
ΣΣ
ΣF
y
the ycomponent of acceleration
The sum of the zcomponents of Forces
Σ
ΣΣ
ΣF
z
the zcomponent of acceleration
Σ
ΣΣ
ΣF
x
causes a
x
Σ
ΣΣ
ΣF
y
causes a
y
Σ
ΣΣ
ΣF
z
causes a
z
Review
affects ONLY
affects ONLY
affects ONLY
The relationship be tween
Forces on an object and
Acceleration of an object
was found to be amazingly simple
The x component of accelerati on of an object
is proportional to
the sum of the x compone nts of all of the
forces on that object from the interactions of
all other objects.
The constant of prop ortionality is
The mass of the object
Forces and Motion
The same is true for the y and z components
Σ
ΣΣ
ΣF
x
= m a
x
Σ
ΣΣ
ΣF
x
= m a
x
Σ
ΣΣ
ΣF
y
= m a
y
Σ
ΣΣ
ΣF
z
= m a
z
Where x, y, z are three
perpendicular direc tions.
all other objects
"your" object with
m is the mass of “your” objec t
Σ
Σ Σ
Σ F = m a
a is the acceleration of "your" object
Σ
Σ Σ
Σ F = m a means:
V
ector Notation
Known as Newton’s 2nd Law
Σ
ΣΣ
ΣF is the sum of the interactio ns of
pf3
pf4
pf5

Partial preview of the text

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This Week

Textbook -- Read Chapter 4, 5Competent Problem Solver - Chapter 4

Pre-lab Computer Quiz

What’s on the next Quiz?

Kinematics - EverythingForces - to lecture before quiz

Check Your Understanding atend of each Laboratory is agood guide

Work problems as if taking the quiz:

Assigned homework - minimumif you can do them easilyProblems at end of chapter 3 and 4of CPS

Check out sample quiz on web by Thurs.

Other textbook problems

What you missed on first quiz

The combined effect of ALL forces on anobject that determines its acceleration.The effects of forces in perpendiculardirections are independent

Forces are vector quantitiesCombining Forces means Vector Addition

Theory of Forces

The Mathematics:

Define a coordinate systemwith perpendicular x and y axes

Add x components of forces

and independently

Add y components of forces

+y

+x F

1

F

2

Example: 2 forces act on an object, howdoes it move?

+y

+x

F

1

F

2

Adding Forces

F = F

1

+ F

2

means

F

x

= F

1x

+ F

2x

and

F

y

= F

1y

+ F

2y

F

1x

F

2x

+y

+x

ΣΣΣΣ

F

x

=F

1x

  • F

2x

F

1y

F

2y

Σ Σ

Σ Σ

F

y

=F

1y

  • F

2y

ΣΣΣΣ

F

θθθθ

F

F

x

2

F

y

2

tan

θ θ

θ θ =

F

y

F

x

First: Take the vectors apart

Second: Put the resulting vector together

The sum of the x components of Forces

F

x

the x component of acceleration

The sum of the y components of Forces

F

y

the y component of acceleration

The sum of the z components of Forces

F

z

the z component of acceleration

F

x

causes a

x

F

y

causes a

y

F

z

causes a

z

Review

affects ONLY affects ONLY

affects ONLY

The relationship between

Forces on an object andAcceleration of an object

was found to be amazingly simple The x component of acceleration of an object

is proportional to

the sum of the x components of all of theforces on that object from the interactions ofall other objects.

The constant of proportionality is

The mass of the object

Forces and Motion

The same is true for the y and z components

F

x

= m a

x

F

x

= m a

x

F

y

= m a

y

F

z

= m a

z

Where x, y, z are threeperpendicular directions.

all other objects

"your" object with

m is the mass of “your” object

F = m a

a is the acceleration of "your" object

F = m a

means:

Vector Notation

Known as Newton’s 2nd Law

F is the sum of the interactions of

If an object is accelerating

Is there always a force in thedirection of the acceleration?

(a) Yes(b) No

If no, give an example

m

F

1

F

2

a

There is no “real” force in the direction of a

Analyze the Forces

Finding all of the forces and their values

Use diagrams to clarify

Simple case: A book on a table

Draw all relevant forces.Did you get them all?How do they combine?How are they related?

Isolate the object you are interested in

Free-body Diagram of Book

Draw only the forces on that object

Only those forces determine its acceleration

First Object: the book

Step 1: Isolation

There appear to be 2 important objects here:

The book

The table

Only the forces on the book

W

b

N

tb

W

b

: gravitational pull of the

Earth on the book (weight ofthe book)N

tb

: contact push of the table

on the book (perpendicular tothe table/book contact)

Free-body Diagram of Table Second Object: the table One more relevant Object: the Earth

W

t

N

bt

N

Et

W

t

: gravitational pull of

the Earth on the table(weight of the table)

N

bt

: contact push of

the book on the table(perpendicular to thebook/ table contact) N

Et

: contact push of the

ground on the table(perpendicular to theground/table contact)

Contact pushes by a surface are usuallycalled normal forces

Normal is an old fashioned wordfor perpendicular

Third Object: the EarthFree-body Diagram of Earth

W

bE

: gravitational pull of

the book on the Earth

W

tE

: gravitational pull of

the table on the Earth

N

tE

: contact push of the

table on the ground(perpendicular to theground/table contact)

W

bE

W

tE

N

tE

How are these forces related to each other?

Relationship of Forces on

a Single Object

For the book:

F

y

= m a

y

W

b

N

tb

N

tb

- W

b

N

tb

= W

b

For the table:

F

y

= m a

y

W

t

N

bt

N

Et

N

Et

= W

t

+ N

bt

W

bE

W

tE

N

tE

For the Earth:

F

y

= m a

y

N

tE

= W

bE

+ W

tE

+y

A 20 kg block rests on a frictionless table. A

cord attached to the block extendshorizontally to a pulley at the edge of thetable. When another block of unknown massis hung at the end of the cord after it passesover the pulley, the hanging block acceleratesdownward at 2.7 m/s

2

and pulls the other

block with it. Calculate the mass of thehanging block and the tension in the cord.

Example

As might be stated in your text

You have been hired as a consultant for anew movie about an expedition to the SouthPole. In one scene, the explorers are on aglacier that comes to an end with a steepcliff. They need to get their supplies downthe cliff. For safety, each box of supplies isroped to another box with a 30 m rope. Onebox breaks away and falls off the cliff. The20 kg box it is roped to is pulled over thehorizontal ice of the glacier towards the edgeof the cliff. It is important that the hero of thestory save this box. You calculate that thiscan be done if this it has an acceleration of2.7 m/s

2

. Now you need to know the mass of

the other box and the necessary strength ofthe rope. As it might appear on a quiz

A

B

Find mass of hanging block andtension in cord

Use forces on B to relate acceleration to m

B

2.7 m/s

2

20 kg

2.7 m/s

2

Question:

Approach: Use forces on A to relate acceleration to T

A

For massless rope T

A

= T

B

m

B

Assumptions: massless cord,

frictionless ice

Since B accelerates, force of rope on B isless than its weight

W

A

N

A

T

A

W

B

T

B

A and B are tied together so they havethe same magnitude of acceleration

You recognizethis from the lab

FOCUS THE PROBLEM

+y

+x

The Massless Rope

A very useful approximation

You pull a block with a rope by exertinga force P and the block accelerates

P

The rope pulls on the block with a force T

T

How are P and T related?

The block pulls on the rope with a force T.

3rd Law Pairs

T

Free body diagram of the rope

P

T

F = m

rope

a

F = 0

Approximate m

rope

Thus T = P

The force exerted on the rope equals the forcethe rope exerts on the block

a

a

Free-body Diagram of A

W

A

N

A

T

Force Diagram of A

+y

+x

W

A

N

A

T

Relevant Equations:

F

x

= m a

x m

A

= 20 kg

a

B

= 2.7 m/s

2

Target quantities: m

B

and T

Block A

T = m

A

a

N

A

- W

A

Block B

T - W

B

= m

B

(-a)

Free-body Diagram of B

T

W

B

Force Diagram of B

+y

+x

T W

B

a

a

W = mg

Physics Description

F

y

= m a

y

Find T

Find m

B

unknowns

consider the motion of object B.

m

B

W

B

= m

B

g

T, W

B

Find W

B

-m

B

a = T - m

B

g

Must consider object A to getmore information

T - W

B

= m

B

(-a)

For object A

T = m

A

a

Note: 3 unknowns, 3 equations

ok

Plan the Solution

(20kg) (2.7 m/s )

2

2

2

(9.8 m/s - 2.7 m/s )

m

B

7.6 kg

m

B

Now for the other target, T

Looking at the mathematical plan

equation

T = m

A

a

T = (20 kg) (2.7 m/s )

2

T = 54 kg m/s

2

= 54 N

m

A

a - m

B

g = -m

B

a

m

A

a = m

B

g - m

B

a

m

A

a = m

B

(g - a)

Check units

accel. units cancelgiving mass units, ok

m

A

a

(g - a)

= m

B

Execute the Plan

Putting [3] and [2] into [1]

Is it properly stated?

Quantities in the mathematics aredescribed in the picture

Quantities solved for have appropriate units

Is it unreasonable?Since B accelerates downward,

T < W

B

W

B

= m

B

g

W

B

= 7.6 kg (10 m/s )

2

W

B

= 76 N

54 N < 76 N

Is it complete?

Yes, found both T and m

B

mass in Kgforce in N

The mass of B (7.6 kg) is reasonable for asmall box

Evaluate the Solution

This is reasonable

As the engineering advisor to anarcheological team, you are trying to figureout how the ancient Egyptians could lift largeblocks of stone from a quarry. The team hasfound evidence of wooden disks which couldhave been used as pulleys. The team leaderhas suggested that a three pulley system withone fixed pulley and two movable pulleysmight have been used. You to have beenassigned determine if the ropes used by theEgyptians would have been strong enoughfor such a system to lift a 1000 kg block ofstone using the pulley system sketchedbelow. You also want to know if one personcould lift a block using that system.

Example

T

2

T

1

T

4

M

What is the force on each rope?

Assume massless ropes

A

B

C

+y

+x

Assume frictionless, massless pulleys

1000 kg

Question:Approach

F

y

on each pulley is 0 (no acceleration)

Assume that block is pulled up ata constant velocity.

There are 4 ropes in the problem

Use Newton’s 3rd Law to relate forceexerted on a rope to force exerted by therope by other objects.

What is force needed to lift block?

Objects are: block and 3 pulleys

Focus

P T

3

Free - body diagrams

T

1

W

T

2

T

2

T

1

A

T

2

T

3

T

3

B

T

4

T

3

T

3

C

Block

Pulley A

Pulley B

Pulley C

M = 1000 kga = 0

Target variables: T

1

, T

2

, T

3

, T

4

Relevant Equations:

F

y

= m a

y

Block: T

1

- W = 0

Pulley A: 2T

2

- T

1

Pulley B: 2T

3

- T

2

Pulley C: T

4

- 2T

3

W = Mg

Describe the Physics

Find T

1

T

1

  • (-Mg) = 0

Find T

3

consider the motion of the block

unknowns

T

1

Find T

2

T

2

consider the motion of pulley A

consider the motion of pulley B

T

3

T

1

= M g

2 T

2

-T

1

2T

3

-T

2

T

2

= Mg/

T

3

= Mg/

Find T

4

consider the motion of pulley C

T

4

T

4

- 2T

3

T

4

= Mg/

Plan

Riding in a friend’s sports car you feel the

seat pushing on your back when it pulls awayfrom a stop light. You decide you want toknow the 1000 kg car’s acceleration. Howmany g's are you "pulling"? You notice thereis a die hanging from the rear view mirror.Very retro. When the car leaves theintersection the die makes an angle of 15 °with the vertical. Later you measure themass of that die to be 100 grams. What wasthe acceleration of the car?

Example

15°

T

a

Are we sure thatthe angle of thedie is as drawn?

Picture

Mass of die : 100 gramsMass of car: 1000 kg

What is the acceleration of car?

Initial velocity of car : 0

Question:Approach:

Acceleration of car is acceleration of die

Relate acceleration to force on the die Consider forces on die

By Earth (Weight)By string (tension)

The acceleration in one direction isindependent of the forces in perpendiculardirections

Use components

Focus

W

Free body diagramof die

T

W

W

Force diagram of die

T

θθθθ

+y

  • x

m = 100 gr

a

y

F

x

= m a

x

F

y

= m a

y

W = m g

target variable: a

x

Relevant equations:

T

x

= ma

x

T

y

  • W = ma

y

sin

θθθθ

T

x

T

cos

θ θ

θ θ

T

y

T

tan

θθθθ

T

x

T

y

Physics Description

T

x

T

y

Find a

x

Horizontal motion of the die

unknowns

a

x T

x

Find T

x

T

T

x

= ma

x

tan

θθθθ

T

x

T

y

Find T

y

T

y

  • mg = 0

T

y

3 unknowns, 3 equations

done

T

y

= mg

tan

θθθθ

T

x

mg

mg tan

θθθθ

= T

x

mg tan

θθθθ

= ma

x

g tan

θθθθ

= a

x

Execute:

a

x

tan (15°) g

a

x

= 0.27 g

Plan

Vertical motion of the die

a

x

is in same units as g which is an

acceleration so units are correctThe question is answered since thecar is accelerating in the x directionand the die is moving with the car.A car which goes from 0 to 50 mph in10 seconds has a high acceleration

v

a

av

t

a

av

mihr

sec

This car’s acceleration is about that so theanswer is reasonable

Is the answer unreasonable?

mi

hr

ft

mi

hr

min

min

sec

10 sec

a

av

since g = 32 ft

sec

2

a

av

7 ft

sec

2

< 1/4 g

Evaluate