All AP Physics 1 Resources
Example Questions
Example Question #491 : Ap Physics 1
A locomotive of mass traveling at couples to a motionless passenger car without applying the brakes. Assuming no momentum losses, calculate the final velocity.
None of these
Use conservation of momentum
Plug in values:
Solve for :
Example Question #31 : Impulse And Momentum
A tennis player hits an incoming tennis ball of mass and speed right back at his opponent at a speed of in the exact opposite direction. Suppose the collision between the racket and the tennis ball lasted for .
What is the magnitude of the average force exerted by the racket on the tennis ball?
The average force exerted by the racket is related to the impulse by
The impulse is related to the change in momentum by
Equating the two expressions for impulse gives us
Simplify to get
The change in velocity is given as
Plugging in this, along with the given change in time and mass of the tennis ball gives us:
Since the question asks for the magnitude of the average force, we get rid of the negative above to obtain
Example Question #32 : Impulse And Momentum
A car takes to accelerate to from rest. Determine the average force experience by a driver of mass .
Use the equation for momentum:
Initial velocity was
Plug in values:
Example Question #31 : Impulse And Momentum
A popular topic in early space exploration was how to safely return modules back to the surface of the earth. Early designs contained materials that could only withstand impulses of up to before parts of the module became compromised. One such model of mass 500kg is approaching ocean waters and deploys its shoot, reducing its speed to . If the module decelerates to zero velocity in 0.9 seconds upon hitting the water, is the module structurally compromised?
No; the impulse experienced is
More information is needed to solve
Yes; the impulse experienced is
Yes; the impulse experienced is
No; the impulse experienced is
No; the impulse experienced is
We need to use the equation for impulse to solve this problem. In fact, the time given is completely irrevelevant:
Plugging in our values:
This is less than the threshold, so no, nothing becomes structurally compromised
Example Question #35 : Impulse And Momentum
An arrow with mass is shot straight up in the air with an initial kinetic energy of . What is the momentum of the arrow after . Neglect air resistance.
In order to determine the momentum of the arrow, we are going to need its velocity at that time. First, we will convert the initial kinetic energy into initial velocity:
Rearranging for velocity:
Then we can use the following equation to calculate the velocity after 1 second:
Then using the expression for momentum:
Example Question #31 : Impulse And Momentum
Conservation of momentum, , is true for which scenario?
Momentum is conserved if all forces, , are conservative.
Momentum is conserved only in one-dimensional collisions.
Momentum is conserved if no net external force, , is present.
Momentum is always conserved.
Momentum is conserved if no net external force, , is present.
Momentum is conserved in isolated systems, (i.e. there are no net external forces.)
Example Question #33 : Impulse And Momentum
Determine the momentum of a baseball of mass moving at .
None of these
Using the equation for kinetic energy
Converting to and plugging in values:
Example Question #34 : Impulse And Momentum
Two cars of mass hit head on, each traveling at . They then bounce back at If the collision took , determine the magnitude of force experienced by each car.
Impossible to determine
None of these
Using momentum principle:
Since the cars have identical masses and experience the same change in velocity, the forces on them will be identical.
Plugging in values:
Solving for :
Example Question #37 : Impulse And Momentum
Two cars of mass hit head on, each traveling at . They then bounce back at If the collision took , determine the force experienced by a driver of mass in one of the cars.
Impossible to determine
None of these
Using momentum principle:
Since the cars have identical masses and experience the same change in velocity, the forces on them will be identical.
Plugging in values:
Solving for :
Now, determine the acceleration of the car:
Now, determine the force experienced by the driver who was in the car, and thus accelerated with the car.
Example Question #33 : Impulse And Momentum
When firefighters rescue a person from a burning building several stories high, they're prepared with a padded landing for when the person jumps down. As this person falls, they build up greater and greater momentum. How does the padded landing bring this falling person safely to rest?
It decreases the force of the collision by decreasing the time of the collision
It increases the force of the collision by decreasing the time of the collision
It increases the force of the collision by increasing the time of the collision
It decreases the force of the collision by increasing the time of the collision
It decreases the force of the collision by increasing the time of the collision
For this question, we're asked how a padded landing helps a person fall safely from a large height. To do so, we need to consider how the landing interacts with the falling person in changing their momentum.
Let's first remember that a change in an object's momentum is called impulse, which can be written with the following expression.
What's more, the units can be rearranged in such a way as to express impulse in terms of average force and time of the collision.
Next, we can rearrange the above expression to make it easier to see how force and time of collision are related.
As we can see in the above expression, the average force of collision is inversely proportional to the time of the collision. In other words, the longer the collision lasts, the less the average force will be.
Relating this to the padded landing example, it's clear that the landing helps to reduce a person's fall by reducing the average force of the collision between the person and the landing. Moreover, the amount of time the collision takes to happen is increased.
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