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Example Questions
Example Question #1 : Contact Forces
A box is released on a 25 degree incline and accelerates down the ramp at . What is the coefficient of kinetic friction impeding its motion?
Consider the net forces acting on the object causing it to accelerate.
To determine the Force of Gravity in the x-direction, we must break the force of gravity into components and examine the side acting in the x-direction. Using trigonometric functions we get that
We know that the force of gravity is equal to mg
According to Newton’s 2nd law the force is equal to the mass times the acceleration of the object.
The force of friction is directly related to μ (the coefficient of friction) times the normal force. In this case the normal force is equal to the y component of the force of gravity.
Therefore
If we substitute this in our original net force equation
Notice that mass is in each piece of the equation so we can cancel it out.
Now we can rearrange and solve for the coefficient of friction
Example Question #3 : Contact Forces
Two toy cars (15kg and 3kg) are released simultaneously on an inclined plane that makes an angle of 28 degrees with the horizontal. Which statement best describes their acceleration once they are released. Assume that the track is frictionless.
None of the above
The 3kg car accelerates 5 times faster than the 15kg car
The 15kg car accelerates 5 times faster than the 3kg car
Both cars accelerate at the same rate
Both cars accelerate at the same rate
Since the only force pulling both cars down the slope is the force of gravity, both cars will accelerate at the same rate.
It is possible to prove this mathematically by examining the x-component of the gravitational pull.
We know that the force of gravity is equal to mg
According to Newton’s 2nd law the force is equal to the mass times the acceleration of the object.
Both sides have mass so this cancels out of the equation.
Since this is independent of mass, this will be true for both objects.
Example Question #4 : Contact Forces
A horizontal force accelerates a box from rest across a horizontal surface where friction is present at a constant rate. Then the experiment is repeated. All conditions remain the same with the exception that the horizontal force is doubled. What happens to the box’s acceleration.
It increases to exactly double its original value
It increases somewhat
It increases to less than double its original value
It increases to more than double its original value
It increases to more than double its original value
According to Newton’s 2nd Law the net force on the object is equal to the mass times the acceleration. The net force is also equal to the sum of the forces involved.
In the second experiment the horizontal applied force is doubled. However, this does not have any effect on the friction on the object. Therefore the new equation is
From this equation we can see that the new acceleration will be more than double the original value.
To examine this numerically, let’s assume that the mass of the box is , the friction force is and the applied force originally was .
Then, let’s double the horizontal force, keeping the friction force the same.
This value is more than double the original value, confirming our answer.
Example Question #5 : Contact Forces
A block is on a smooth horizontal surface (), connected by a tine cord that passes over a pulley to a second block which hangs vertically (). Find the formula for the acceleration of the system. Ignore friction and the masses of the pulley and cord.
Cannot determine this with the information provided
To determine the net force on a system, it is important to consider all the forces between each object in the same direction. The direction to be considered is along the line of the rope. The system is considered to be all the blocks together as they will all move with the same acceleration.
According to Newton’s 3rd Law, the Tension in the rope caused by A pulling on B and B pulling on A is equal in magnitude and opposite in direction. Therefore these two Tension forces cancel out.
From Newton’s 2nd law we know that the net force on a system is equal to the mass of the system times the acceleration of the system
Therefore
We can calculate the force of gravity from the equation Fg = mg
Therefore
We can rearrange this equation and solve for a
Example Question #3 : Contact Forces
Susan is trying to push a crate across the floor. She observes that the force of friction between the crate and the floor is . What is the coefficient of static friction? Assume
It cannot be determined
The equation for the force of friction is , where μ is the coefficient of static friction.
The normal force is equal to the mass times acceleration due to gravity, but in the opposite direction (negative of the force of gravity).
Since the problem tells us that the force due to friction is , we can plug these values into our original equation to solve for the coefficient of friction.
The coefficient of friction has no units.
Example Question #6 : Contact Forces
Which of the following cannot be true of an object on a given surface?
Static friction: Kinetic friction:
Static friction: Kinetic friction:
Static friction: Kinetic friction:
Static friction: Kinetic friction:
Static friction: Kinetic friction:
Static friction: Kinetic friction:
Kinetic friction is never greater than static friction. More force is always requires to overcome static friction than is required to overcome kinetic friction. It can require a large force to initiate motion, causing an initial acceleration by overcoming static friction. Once motion has begun, however, less for is required to maintain the motion due to the principles of Newton's first law and inertia.
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