Physical Science 9
Practice Test for Forces Solutions
N1:
If an object is experiencing an acceleration (or change in velocity, or change
in speed and/or direction) it must have a net force on it. Likewise, if it does not have a net
force on it, it will not accelerate.
Example: Consider the moon orbiting in a circle around
the earth at constant speed. Though
its speed is not changing its direction is, so it is accelerating, hence it
must have a net force on it.
N2: An
object of mass m will experience an acceleration a when a net force Fnet
is applied to it, such that:
Fnet= ma (the net force points in the same direction as the
acceleration).
Example: If I (of mass 75 kg) were in outer
space, away from any planet or star, and was being pulled by a rope with
tension 100N to the right and a rope of tension 250N to the left I would feele
a net force to the left of 150N.
From N2 I can calculate my acceleration algebraically as:
a = Fnet/m
in this case it will give:
a = 150N left / 75 kg = 2.0 m/s2 left
N3: If object 1 feels a force from object 2 (the
action) then object 2 will experience the same size force from object 1 but in
the opposite direction (the reaction).
Example: If I am standing on the ground and
the ground pushes up on me with a normal force of 735N then I will push down on
the ground with a normal force of 735N.
The brick will have two arrows of
force: an arrow pointing down from its center labeled “W” or “weight” or “force
of gravity” which will be equal to W = mg = 0.80kg×9.8 m/s2 =
7.84 N and an arrow pointing up from the bottom of the brick labeled “N” or “normal
force”. The normal force must be
equal to the weight since the brick is not moving so it has zero acceleration
(from N1 and/or N2). So, you label
the normal force with 7.84N as well.
The reaction forces will be:
To the normal force: the brick will push down on the ground
with 7.84 N.
To the weight: the brick will pull
up on the earth with a gravity force of 7.84 N.
There will be a normal force
directed from the surface of contact between the ball and the ground point out
at right angles from the hill.
There will be a frictional force
from the surface of contact backward along the hill.
There will be a weight force from
the center of the ball directed down.
Since it
has constant speed and direction it has no acceleration and hence no net
force. The 200N towing the car
must be balanced by 200N of friction resisting the pull.
If the cars hits a patch of oil and the force of friction reduces to 100N, what would the acceleration of the car be?
Now the
net force will be 100N in the direction it is being towed (200N towing force
minus 100N friction force). From
N2:
a = Fnet/m
=
100N/2000kg = 0.050 m/s2 in the direction of towing.
(Bonus: if the car is traveling at 10m/s when it hits the oil patch, how fast will it be traveling 2.0 s later?)
From last
unit the equation for acceleration is:
a = Δv/Δt
so Δv
= a Δt
Here we have a=0.050 m/s2
and Δt = 2.0s from the question so:
Δv = 0.050 m/s22.0s
= 0.10m/s in the direction of towing.
If it starts at 10m/s in the
direction of towing and GAINS 0.10m/s it will have 10.1m/s in the direction of
towing.
It’s up to you!