All AP Physics 1 Resources
Example Questions
Example Question #1 : Forces
Consider the following system:
If , what is the minimum coefficient of static friction that will keep the block stationary?
There are two forces at play in this scenario: the force of friction and the force of gravity. If the block is stationary, that means that the two forces cancel each other out. Therefore, we can write:
Substituting in expressions for each force, we get:
If you are unsure of whether to use cosine or sine for each force, think about the situation practically. The flatter the slope gets, the less the force of gravity will have an effect on trying to move the block down the plane, hence the use of the sine function. Also, the flatter the slope gets, the greater the normal force will become, hence the use of the cosine function.
Example Question #1 : Forces
Consider the following system:
Side is equal to , yet the block travels down the slope with an acceleration of . If , what is the coefficient of kinetic friction?
There are two forces in play in this scenario: gravity and friction. We can use Newton's second law to form an expression with these forces:
Substituting in expressions for each force, we get:
If you are unsure of whether to use cosine or sine for each force, think about the situation practically. The flatter the slope gets, the less the force of gravity will have an effect on moving the block down the plane, hence the use of the sine function. Also, the flatter the slope gets, the greater the normal force will become, hence the use of the cosine function.
Canceling out mass and rearranging for the coefficient of friction, we get:
Example Question #2 : Normal Force And Weight
Consider the following system:
If the normal force on the block is and the angle of the slope is , what is the mass of the block?
We need to develop an expression for the normal force on the block to solve this problem:
If you are unsure of whether to use sine or cosine, think about the system practically: the flatter the system gets, the larger the normal force will become; hence the use of the cosine function.
Rearranging for mass, we get:
Example Question #3 : Forces
What is the magnitude of the normal force exerted on an an object weighing 5kg, which is on a incline to the horizontal?
Cannot be determined without knowing the height of the object from the ground
Recall that the formula for determining the magnitude of the normal force on an incline is given by:
Here, is the magnitude of the normal force, is the mass of the object, is the gravitational constant, and is the angle made with the horizontal.
In our case:
Example Question #1 : Forces
An object with a mass of 10kg is resting on a horizontal table. What is the normal force acting on the object?
The normal force points perpendicular to the force of gravity (opposite direction) and is equal in magnitude. Because the force of gravity is equal to , we simply multiply our given mass and the force of gravity to get our answer.
Example Question #2 : Forces
A person who weighs is standing in an elevator. The elevator then accelerates upward at a rate of . During this acceleration, how much does the person weigh?
The person's weight will not change, it will remain at
There is not enough information given to solve this problem
In this question, we're presented with a scenario where a person weighing at rest is being accelerated upwards. We're then asked to determine this person's new weight while they are undergoing this acceleration.
Let's begin our analysis by first considering the person to be at rest in the elevator. In this situation, it's useful to picture a free-body diagram of the person and all of the forces acting on him/her. While at rest, there is no net force acting on this individual. Since there is no net force in the y-direction, that means that the upward forces must be exactly balanced by the downward forces. The downward force acting on the individual is the force due to gravity, while the upward force is the normal force of the elevator's floor acting on the individual.
Put another way:
Next, let's derive an expression while considering the upward acceleration of the elevator. In such a situation, there is now a net force acting on the individual, and that net upward force is due to the elevator's acceleration. Just as it was while at rest, the downward force acting on the individual in this case is still the force due to gravity, and the upward force acting on the individual is the normal force of the elevator's floor.
Written in equation form, we have:
Notice that we are solving for the new value of the normal force while the elevator is accelerating. The reason why the normal force gives us the person's weight is due to Newton's third law. When the elevator accelerates upward, the elevator exerts a (normal) force on the individual that is equal in magnitude to the person's weight, but with reversed directionality.
Finally, we can calculate the person's mass:
Plugging the relavent values into the above expression that we've derived will give us our answer.
Notice that this value is greater than the that the person weighs while at rest. This is due to Newton's first law. When the elevator accelerates upward, the person's inertia resists this upward movement, which makes the person feel heavier. You can actually try this out for yourself next time you find an elevator!
Example Question #572 : Newtonian Mechanics
You are in a small spacecraft that has no windows traveling through space. The craft is accelerating and you have a bathroom scale at your disposal. Before you left Earth that morning you weighed yourself to be . You step on the scale and find it reads . How fast is the craft accelerating in ?
None of these
One thing to note is that the weight measured was given in pounds instead of Newtons. We could convert the weights, but it turns out that we don't need to.
If your weight measured on Earth is
and the weight on the craft is
we know that on Earth the acceleration is . Using Newton's second law,
and
we can set equal since the mass never changes only the weight force, and solve for ,
This makes sense that you would weigh more if you were experiencing a larger acceleration. This is interesting because you could not tell if you were standing stationary in a gravitational field or accelerating in a non-inertial reference frame. This is what is known as the Equivalence Principle.
Example Question #11 : Forces
Determine the gravitational constant on a newly discovered planet, Planet X, if it exerts of force on a piece of rock. on the surface.
Using Newton's second law, we can determine the answer.
In our problem, and . is the acceleration due to gravity. Therefore,
Example Question #12 : Forces
A person steps on a scale and reads that his mass is . The person then steps on the scale while on a plane that is inclined at . What is the new mass reading on the scale?
The reading on a scale is really the normal force . On a flat surface, we see the person has a reading of , or . On an inclined surface, one can show that the normal force has a new magnitude of:
This will lead the scale to read read:
Example Question #13 : Forces
An astronaut of mass is on a space craft blasting off from the surface of the earth. after blast off, the acceleration of the ship is . Determine the force the astronaut experiences from her seat at this moment in time.
None of these
Plug in values:
Solve for :
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