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Transcript
Monday Jan 18
Answers q 1-4 pg 132
1a) 12N b) 3.0 m/s2
2) The reaction force acts on the child, not on the wagon itself, so there is still a
net force on the wagon.
3 A) person pushes on ground; ground pushes on person
B) snowball exerts a force on back; back exerts force on snowball
C) ball exerts a force on glove; glove exerts a force on ball
D) wind exerts a force on window; window exerts a force on wind
4) 1.6 m/s2 at an angle of 65 degrees north of east

Define weight and explain how it differs from mass.
Weight: a measure of the gravitational force exerted on an object; its value can
change with the location of the object in the universe.
Mass: is a measure of the amount of matter in an object. It is an inherent property of
an object.

Define normal force and explain why friction is proportional to the normal force.
Normal Force: the force that acts on a surface in a direction perpendicular to the
surface.
Both the normal force and friction are dependent on mass. Experimental findings have
shown that the normal force and friction force are proportional.

Define static friction, kinetic friction and the coefficient of friction.

Static friction: force that resists the initiation of sliding motion between two
surfaces that are in contact and at rest

Kinetic friction: the force that opposes the movement of two surfaces that are in
contact and in motion

Coefficient of friction: the ratio of the magnitude of the force of friction to the
magnitude of the normal force (between two objects in contact)
Page 137 Q1-3
On a piece of paper to hand in:

Draw a free body diagram of:

A) a tv sitting at rest

B) a 400 kg elephant sitting on a ramp elevated at 10 degrees from the
horizon
Example problem pg 138
Chapter 4
Section 4 Everyday Forces
Sample Problem
Overcoming Friction
A student attaches a rope to a 20.0 kg box of books.He pulls with a force
of 90.0 N at an angle of 30.0° with the horizontal. The coefficient of
kinetic friction between the box and the sidewalk is 0.500. Find the
acceleration of the box.
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Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Section 4 Everyday Forces
Sample Problem, continued
1. Define
Given:
m = 20.0 kg
k = 0.500
Fapplied = 90.0 N at  = 30.0°
Unknown:
a= ?
Diagram:
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Section 4 Everyday Forces
Sample Problem, continued
2. Plan
Choose a convenient coordinate system, and
find the x and y components of all forces.
The diagram on the right shows the
most convenient coordinate system,
because the only force to resolve
into components is Fapplied.
Fapplied,y = (90.0 N)(sin 30.0º) = 45.0 N (upward)
Fapplied,x = (90.0 N)(cos 30.0º) = 77.9 N (to the right)
Chapter menu
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Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Section 4 Everyday Forces
Sample Problem, continued
Choose an equation or situation:
A. Find the normal force, Fn, by applying the condition of
equilibrium in the vertical direction:
Fy = 0
B. Calculate the force of kinetic friction on the box:
Fk = kFn
C. Apply Newton’s second law along the horizontal direction to
find the acceleration of the box:
Fx = max
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Section 4 Everyday Forces
Sample Problem, continued
3. Calculate
A. To apply the condition of equilibrium in the vertical direction,
you need to account for all of the forces in the y direction:
Fg, Fn, and Fapplied,y. You know Fapplied,y and can use the box’s
mass to find Fg.
Fapplied,y = 45.0 N
Fg = (20.0 kg)(9.81 m/s2) = 196 N
Next, apply the equilibrium condition,
Fy = 0, and solve for Fn.
Fy = Fn + Fapplied,y – Fg = 0
Fn + 45.0 N – 196 N = 0
Fn = –45.0 N + 196 N = 151 N
Tip: Remember to
pay attention to the
direction of forces.
In this step, Fg is
subtracted from Fn
and Fapplied,y
because Fg is
directed downward.
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Section 4 Everyday Forces
Sample Problem, continued
B. Use the normal force to find the force of kinetic friction.
Fk =  kFn = (0.500)(151 N) = 75.5 N
C. Use Newton’s second law to determine the horizontal
acceleration.
Fx  Fapplied  Fk  max
ax 
Fapplied, x  Fk
m
77.9 N  75.5 N
2.4 N
2.4 kg  m/s2



20.0 kg
20.0 kg
20.0 kg
a = 0.12 m/s2 to the right
Chapter menu
Resources
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Chapter 4
Q1-4 page 139
Section 4 Everyday Forces