Title: Chapter 4- Forces and Motion
1Chapter 4- Forces and Motion
2Think about the following questionsWhat is this
object? Where is it? Why does it look like that?
IO is a moon of Jupiter Competing forces between
Jupiter and the other Galilean moons cause the
center of Io compress and melt. Consequently
Io is the most volcanically active body in the
solar system.
3Other examples of forces
4What is a force?
- IPC definition A push or a pull exerted on some
object - Better definition Force represents the
interaction of an object with its environment - The Unit for Force is a Newton
5Two major types of forces
- Contact Forces Result from physical contact
between two objects - Examples Pushing a cart, Pulling suitcase
- Field Forces Forces that do not involve physical
contact - Examples Gravity, Electric/Magnetic Force
6Force is a vector! (yay more vectors ?)
- The effect of a force depends on magnitude and
direction
7Force Diagrams (p. 126)
- Force Diagram A diagram that shows all the
forces acting in a situation
8Free Body Diagrams p.127
- Free Body Diagrams (FBDs) isolate an object and
show only the forces acting on it - FBDs are essential! They are not optional! You
need to draw them to get most problems correct!
9How to draw a free body diagram
- Situation A tow truck is pulling a car
- (p. 127)
- We want to draw a FBD for the car only.
10Steps for drawing your FBD
- Step 1 Draw a shape representing the car (keep
it simple) - Step 2 Starting at the center of the object,
Draw and label all the external forces acting on
the object
11Add force of gravity
12Add force of the road on the car(Called the
Normal Force)
13Finally add the force of friction acting on the
car
14A Free Body Diagram of a Football Being Kicked
15A person is pushed forward with a force of 185 N.
The weight of the person is 500 N, the floor
exerts a force of 500 N up. The friction force is
30 N.
16Forces you will need
Symbol of Force Description
Fg Gravitational Force is the Weight of the Object (equal to mass x g mg)
FN Normal Force Force acting perpendicular to surface of contact
Ff Frictional Force- Opposes applied force acts in direction opposite of motion
Fapp Applied Force
17Sample Problem p. 128 3
- Draw a free body diagram of a football being
kicked. Assume that the only forces acting on the
ball are the force of gravity and the force
exerted by the kicker.
18Newtons 1st Law of Motion
- The Law of Inertia
- An object at rest remains at rest, and an object
in motion continues in motion with constant
velocity (constant speed in straight line) unless
the object experiences a net external force - The tendency of an object not to accelerate is
called inertia
19Acceleration
- The net external force (Fnet) is the vector sum
of all the forces acting on an object - If an object accelerates (changes speed or
direction) then a net external force must be
acting upon it
20Equilibrium
- If an object is at rest (v0) or moving at
constant velocity, then according to Newtons
First Law, Fnet 0 - When Fnet 0, the object is said to be in
equilibrium
21How do we use this information?Sample Problem p.
133 2
- A crate is pulled to the right with a force of
82.0 N, to the left with a force of 115 N, upward
with a force of 565 N and downward with a force
of 236 N. - A. Find the net external force in the x direction
- B. Find the net external force in the y direction
- C. Find the magnitude and direction of the net
external force on the crate.
22Step 1 Draw a FBD
Fup 565 N
Fright 82 N
Fleft 115 N
Fdown 236 N
23Find the vector sum of forces
- A. 82 N (-115 N ) -33 N
- B. 565 N (-236 N) 329 N
- C. Find the resultant of the two vectors from
part a and b.
24Newtons 1st Law
- Review Newtons 1st Law
- When Fnet0, an object is in equilibrium and will
stay at rest or stay in motion - In other words, if the net external force acting
on an object is zero, then the acceleration of
that object is zero
25Newtons 2nd Law (p.137)
- The acceleration of an object is directly
proportional to the net external force acting on
the object and inversely proportional to the
objects mass
26Example p. 138 4
- A 2.0 kg otter starts from rest at the top of a
muddy incline 85 cm long and slides down to the
bottom in 0.50 s. What net external force acts on
the otter along the incline?
27Solving the problem
- To calculate Fnet, we need m and a
- M2.0 kg
- What is a?
- Vi 0 m/s, t0.50 s,
- displacement85 cm.85 m
- Welcome back kinematic equations! ?
28(No Transcript)
29Newtons 3rd Law
- Forces always exist in pairs
- For every action there is an equal and opposite
reaction
30Action- Reaction Pairs
Some action-reaction pairs
31Although the forces are the same, the
accelerations will not be unless the objects have
the same mass.
32Everyday Forces
- Weight Fg mg
- Normal Force FN Is always perpendicular to the
surface. -
- Friction Force Ff
- Opposes applied force
- There are two types of friction static and
kinetic
33Static Friction
- Force of Static Friction (Fs) is a resistive
force that keeps objects stationary - As long as an object is at rest
- Fs -Fapp
34Kinetic Friction
- Kinetic Friction (Fk) is the frictional force on
an object in motion
35Coefficients of Friction
- The coefficient of friction (µ) is the ratio of
the frictional force to the normal force - Coefficient of kinetic Friction
- Coefficient of Static Friction
36Sample Problem p. 145 2
- A 25 kg chair initially at rest on a horizontal
floor requires a 365 N horizontal force to set it
in motion. Once the char is in motion, a 327 N
horizontal force keeps it moving at a constant
velocity. - A. Find coefficient of static friction
- B. Find coefficient of kinetic friction
37Coefficient of Static Friction
- In order to get the chair moving, it was
necessary to apply 365 N of force to overcome
static friction. Therefore Fs 365 N. - The normal force is equal to the weight of the
chair (9.81 x 25 245 N)
38Coefficient of Kinetic Friction
- The problem states that the chair is moving with
constant velocity, which means Fnet0. Therefore,
Fapp must equal -Fk.
39Solve for Coefficient of Kinetic Friction
40Forces at an angle
- A woman is pulling a box to the right at an
angle of 30 above the horizontal. The box is
moving at a constant velocity. Draw a free body
diagram for the situation.
41FBD
42What is Fnet?
- Since the suitcase is moving with constant
velocity, Fnet0. - That means the forces in the x direction have to
cancel out and the forces in y direction have to
cancel out - Fk Fapp,x
- FN Fapp,y Fg
- NOTICE THAT NORMAL FORCE DOES NOT EQUAL WEIGHT IN
THIS SITUATION
43Lets do an example. P. 154 42
- A 925 N crate is being pushed across a level
floor by a force F of 325 N at an angle of 25
above the horizontal. The coefficient of kinetic
friction is 0.25. Find the magnitude of the
acceleration of the crate.
44What do we need to know?
- So we need mass and Fnet.
- We have weight (925 N). So what is mass?
- How to find Fnet?
- Find vector sum of forces acting on crate.
45FBD
46Finding Fnet,y
- Is box accelerating in y direction?
- No. Therefore Fnet in y direction is 0
- So FN Fapp,y Fg
- So FN Fg- Fapp,y 925 N- 325sin(25)
- FN 787.65 N
47Finding Fnet,x
- Is box accelerating in x direction?
- Yes. Therefore Fnet,x is not 0
- Fnet,x Fapp,x Ff
- Fapp,x Fappcos(25)294.6 N
- Use coefficient of friction to find Ff
- FfµFN(0.25)(787N)197 N
48Finish the Problem
- Fnet,x 294 N 197 N 97 N
- So now we know that the Fnet on the box is 97 N
since Fnet,y is 0
49Another example. P. 154 54 part a
- A box of books weighing 319 N is shoved across
the floor by a force of 485 N exerted downward at
an angle of 35 below the horizontal. - If µk between the floor and the box is 0.57, how
long does it take to move the box 4.00 m starting
from rest?
50DRAW FBD
FN
Fapp,x
Ff
Fapp,y
Fg319 N
Fapp 485 N
51Find Fnet
- Is box accelerating in y direction?
- No. Therefore Fnet in y direction is 0
- So FN Fapp,y Fg
- So FN 485sin(35) 319 N 598 N
52Fnet,x
Is box accelerating in x direction? Yes.
Therefore Fnet,x is not 0 Fnet,x Fapp,x
Ff Fapp,x 485cos(35)397.29 N Use coefficient
of friction to find Ff FfµFN(0.57)(598)341
N Fnet, x 397.29- 341 57.29 N
53- So now we know that the Fnet on the box is
- 57.29 N since Fnet,y is 0
- Weight of box is 319 N.
- Find mass by dividing by 9.81
- m 32.52 kg
54Finish the problem
- We want to know how long it takes for the box to
move 4.00 m. - Find vf so that you can solve for t
- Solve for t
55Forces on An Incline
- A block slides down a ramp that is inclined at
30 to the horizontal. Write an expression for
the normal force and the net force acting on the
box.
56Draw a Free Body Diagram
?
57Closer look at gravity triangle.
58Coordinate system for inclined planes
Y axis
X axis
59Fnet in the y direction
- When a mass is sliding down an inclined plane, it
is not moving in the y direction. - Therefore Fnet,y 0 and all the forces in the y
direction cancel out.
60Forces In the y-direction
- So what are the forces acting in the y direction?
- Look at your FBD
- We have normal force and Fg,y
- Since they have to cancel out
- FN mgcos(?)
61Forces in the x direction
- What is the force that makes the object slide
down the inclined plane? - Gravitybut only in the x direction
62Remember that Vectors can be moved parallel to
themselves!!
?
Fg,y
?
Fg,x
63Forces in the x direction
- So what are the forces acting in the x direction?
- Friction Force (Ff) and Gravitational Force
(Fg,x) - If the box is in equlibrium
- Fg,x Ff
- If the box is accelerating
- Fnet Fg,x - Ff
64What if there is an additional applied force?
- Example a box is being pushed up an inclined
plane
Fapp
Fg,x
Ff
Fg,y
?
65In that case
- FN mgcos?
- Fnet Fapp- Fg,x Ff
- If the object is in equilibrium then
- Fapp Fg,x Ff
66An Example p. 153 40
- A 5.4 kg bag of groceries is in equilibrium on an
incline of angle. Find the magnitude of the
normal force on the bag.
67Draw a FBD
Ff
Fg,x
Fg,y
Fg
?
68Solve the Problem
- The block is in equilibrium so
- Fnet0
- Fg,y FNmgcos?(5.4kg)(9.81)cos(15)
- FN51 N
- Additionally, what is the force of friction
acting on the block?
69Find Force of Friction
- Fnet 0
- Fg,x Ff mgsin?5.4(9.81)sin(15)
- Ff 13.7N
70Example p. 147 3
- A 75 kg box slides down a 25.0 ramp with an
acceleration of 3.60 m/s2. - Find the µk between the box and the ramp
- What acceleration would a 175 kg box have on this
ramp?
71FBD
Ff
Fg,x
Fg,y
Fg
?
72What is Fnet?
- They give mass and acceleration
- So Fnet ma 75kg x 3.60 m/s2
- Fnet 270 N
- FN mgcos?
- Fnet Fg,x Ffmgsin? - Ff
73Solve for Ff
- Fnet Fg,x Ffmgsin? Ff
- Ff mgsin? Fnet
- Ff 75kg(9.8)sin(25) 270 N
- Ff 40.62 N
74Finish the Problem
- We are trying to solve for µk