All AP Physics 1 Resources
Example Questions
Example Question #71 : Work, Energy, And Power
Consider the following system:
Two spherical masses, A and B, are attached to the end of a rigid rod with length l. The rod is attached to a fixed point,p, which is at the midpoint between the masses and is at a height, h, above the ground. The rod spins around the fixed point in a vertical circle that is traced in grey. is the angle at which the rod makes with the horizontal at any given time ( in the figure).
The rod is spinning and mass B has an instantaneous linear velocity of . What is the instantaneous linear kinetic energy of mass A?
We only need to know the equation for linear kinetic energy to solve this problem:
In the problem statement, we were told that the instantaneous velocity of mass B was . Since both masses are attached to a rigid rod and spinning in a uniform circle, we know that:
Plugging this into our original equation, we get:
Example Question #71 : Newtonian Mechanics
Consider the following system:
Two spherical masses, A and B, are attached to the end of a rigid rod with length l. The rod is attached to a fixed point, p, which is at the midpoint between the masses and is at a height, h, above the ground. The rod spins around the fixed point in a vertical circle that is traced in grey. is the angle at which the rod makes with the horizontal at any given time ( in the figure).
The rod is initially at rest in its horizontal position. of work were applied toward rotating the rod. When the rod passes through its horizontal position now, what is the instantaneous linear velocity of mass A?
Neglect air resistance and any internal friction forces.
We will be using the equation for conservation of energy:
We can make a few assumptions to cancel out most terms. If we assume that the reference height of this problem when the rod is horizontal is 0, we can remove both potential energies. Also, the rod is initially at rest, so we can remove initial kinetic energy. Thus, we get:
Breaking up kinetic energy for both masses, we get:
Substituting in expressions for linear kinetic energy (you can also do rotational, but will get to the same answer in extra steps. See the end of the solution):
Both velocities are the same, so we can just eliminate the subscripts:
No we just need to rearrange for velocity:
We know each value, so time to plug and chug:
Let's see why it didn't matter which form of kinetic energy we used. Rotational kinetic energy is the following:
Where:
Substituting these back in:
Canceling out radius:
Which is the formula for linear kinetic energy.
Example Question #72 : Work, Energy, And Power
Consider the following system:
Two spherical masses, A and B, are attached to the end of a rigid rod with length l. The rod is attached to a fixed point, p, which is at the midpoint between the masses and is at a height, h, above the ground. The rod spins around the fixed point in a vertical circle that is traced in grey. is the angle at which the rod makes with the horizontal at any given time ( in the figure).
The rod is initially at rest and horizontal. Mass B suddenly disappears and the rod is allowed to rotate freely. Assuming the mass of the rod itself is negligible, what will be the linear velocity of mass A as it passes through its lowest point?
Neglect air resistance and internal friction forces.
We can use the law of conservation of energy to solve this:
Assuming a height of 0 when the mass is at its lowest point we can remove final potential energy. Also, the rod is initially at rest, so we can removed initial kinetic energy. Thus, we get:
Substituting expressions in for each, we get:
We can substitute the following expression in for our initial height:
Canceling out like terms:
Solving for final velocity:
Example Question #71 : Work, Energy, And Power
How much greater is the energy of a car crash at than .
Four times as great
Twice as great
Half as great
The same
Eight times as great
Four times as great
Combining equations:
Example Question #74 : Work, Energy, And Power
Suppose that an object accelerates from to in the absence of friction. How does the energy necessary to achieve this acceleration differ from when the same object accelerates from zero to ?
The energy needed is two times as great
The energy needed is four times as great
The energy needed is three times as great
The mass of the object needs to be given to answer this question
The energy needed is the same in both cases
The energy needed is three times as great
For this question, we need to consider the difference in the amount of energy needed to accelerate an object by a given amount. Since all the energy put into the system is being used to change the object's motion, we can use the work-kinetic energy theorem.
First, let's consider the case where the object accelerates from at rest. We can calculate the amount of energy required by taking note of the final and initial kinetic energy. Even though we don't have the value for the mass of the object, that is okay, because we'll be comparing kinetic energy values in the end. Thus, the term for mass will cancel out.
Next, we can use the same strategy in order to find the energy needed to go from to .
Now, let's see how the two energy values differ.
Thus, the energy required to accelerate the object from to is triple the amount required to accelerate the same object from zero to .
Example Question #75 : Work, Energy, And Power
Deep in space Object has mass and is initially traveling with velocity . At , it collides with Object , which has mass and is initially motionless. The two objects stick together.
Determine the final kinetic energy of the system
None of these
Using
Plugging in values:
The momentum will be the same in the final state, so again using
Solving for velocity:
Plugging in values (the total mass is equal to the combined masses:
Determining magnitude of velocity:
Plugging in values:
Using definition of kinetic energy:
Plugging in values:
Example Question #22 : Kinetic Energy
Deep in space Object has mass and is initially traveling with velocity . At , it collides with Object , which has mass and is initially motionless. The two objects stick together.
Determine the initial kinetic energy of the system.
None of these
Determining magnitude of velocity:
Plugging in values:
Using definition of kinetic energy:
Plugging in values:
Example Question #77 : Work, Energy, And Power
Deep in space Object has mass and is initially traveling with velocity . At , it collides with Object , which has mass and is initially motionless. The two objects stick together.
Determine the final velocity of the two objects.
None of these
Using
Plugging in values:
The momentum will be the same in the final state, so again using
Solving for velocity:
Plugging in values (the total mass is equal to the combined masses:
Example Question #78 : Work, Energy, And Power
During time period , a rocket ship deep in space of mass travels from to . During time period , the rocket fires. During time period , the rocket travels from to .
Time periods , , and took each.
Determine the kinetic energy during time period .
None of these
Combining equations
Converting to and plugging in values:
Example Question #79 : Work, Energy, And Power
During time period , a rocket ship deep in space of mass travels from to . During time period , the rocket fires. During time period , the rocket travels from to .
Time periods , , and took each.
Determine the kinetic energy during time period .
None of these
Combining equations
Converting to and plugging in values: