All AP Physics 1 Resources
Example Questions
Example Question #1 : Newton's Third Law
A book exerts a force of 2N downwards, into a chair that exerts a force of 5N dowwards to the floor it stands on. What is the force that the floor exerts upwards on the chair?
By Newton's third law, for every reaction there is an equal and opposite reaction. The floor must exert a 7N force upwards on the chair for the system to remain at rest. If it exerted less than that, the chair would be accelerating into the floor. This force, exerted by a surface, perpendicular to it, is called the normal force.
Example Question #301 : Forces
A football player, feeling aggressive, is picking on a kid much smaller than himself. The football player asserts: "All of my hours in the weight room prove I can hit you harder than you hit me!" The smaller and more reserved gentleman replies: "Ya of course you can. I'm much weaker than you". Assuming by "hit" they mean "apply a force", are these two correct to think the football player can hit harder? Why?
Yes, Newton's second law says that the football player will cause the smaller gentleman to accelerate to a greater extent. Therefor he exterts a greater force.
Yes, Newton's second law says that football-playing-high-school bullies always hit harder.
No, Newton's third law says that the force two objects act on each other is always EQUAL in magnitude and opposite in direction.
No, Newton's first law says that the force two objects act on each other is always EQUAL in magnitude and opposite in direction.
No, Newton's third law says that the force two objects act on each other is always EQUAL in magnitude and opposite in direction.
The relative mass of two interacting objects does not influence the magnitude of the force that the two objects exert on each other. Newton's third laws states the force must be equal in magnitude. If you're trying to reconcile how a football player is unable to "hit harder" than someone who does not lift weights, the answer lies in Newton's second law.
The football player weighs more and thus experiences a small acceleration. The smaller gentleman experiences a large acceleration due to his relatively small mass. This large acceleration is what we view when we see a large football player hit someone smaller. The football player hardly changes his motion while the smaller person will fly backwards.
Example Question #1 : Newton's Third Law
Describe the phenomenon of a seat belt keeping someone restrained in their seat during a car crash. In other words, why did the person not leave their seat?
Tension force law
Newton's third law
All the laws describe why the person was not ejected from their seat
Newton's first law
Newton's second law
Newton's third law
While all three laws come into play in a car crash only one is specifically responsible for keeping a person restrained in their seat. Just before the crash, the passenger is moving along at the same speed as the car. When the car collides into the other car and decelerates, the person's body continues to move forward. This is Newton's first law, or the law of inertia. But it is Newton's third law that keeps the person from being ejected from their seat. The force of the person's body moving forward was matched by that of the seatbelt. For every action there is an equal and opposite reaction. If the seat belt was unable to "match" the force of the person's body moving forward against it, it would have snapped and the person would have continued forward.
Example Question #301 : Forces
A locomotive is pushing a train at a constant velocity of . How does the force exerted by the locomotive on the train relate to the force of the train on the locomotive?
They are the same in both magnitude and direction
They are the same in magnitude and opposite in direction
They are in opposite directions and have different magnitudes
None of these
They are in the same direction and have the same magnitude
They are the same in magnitude and opposite in direction
This is Newtons's third law. Every action has an equal an opposite reaction. The reason the train is able to move at all is due to the force the locomotive puts on the rails, which enables it to accelerate the cars.
Example Question #1 : Newton's Third Law
Two objects apply forces to each other. The force on one of the blocks as a function of time in the x-direction is , where and are constants. What's the force as a function of time in the x-direction on the other block? Assume no other forces are present besides the forces the objects apply to each other.
By Newton's third law, every action has an equal and opposite reaction. So the force has an equal and opposite force on the other block. Mathematically, this just means to negate the force.
Example Question #302 : Forces
Two men are having a shoving contest, each man pushes the other at the exact same time. Ross pushes Jake with of force and Jake pushes Ross with of force. How much force is exerted on Jake?
The correct answer is because of Newton's Third Law which states that for every action there is an equal and opposite reaction, so when Jake pushes Ross he also exerts the force he uses on himself. With this plus the force Ross exerts on Jake we arrive at our answer of
Example Question #1 : Force Diagrams
Consider the following system:
If the mass accelerates down the plane at a rate of and the angle , what is the coefficient of kinetic friction between the mass and slope?
Before we start using equations, we need to determine what forces are acting on the block in this system. The only relevant forces in this situation are gravity and friction. We are given the acceleration of the block, giving us the tools to find the net force.
Using Newton's second law, we can write:
The force of friction is subtracted because it is in the opposite direction of the movement of the block. Substituting in expressions for each variable, we get:
Canceling out mass and rearranging for the coefficient of kinetic friction, we get:
We have values for each variable, allowing us to solve:
Example Question #2 : Force Diagrams
Consider the following system:
This system is set on a different planet, which has a gravitational constant different from that on Earth. If the angle measures , the coefficient of kinetic friction is , and the block is accelerating at a rate of , what is the gravitational acceleration on this planet?
There are two relevant forces acting on the block in this scenario: gravity and friction. We can use Newton's second law to solve this problem:
Substituting in expressions for each force, we get:
Eliminating mass and rearranging for , we get:
At this point, we can plug in values for each variable and solve:
Example Question #911 : Ap Physics 1
In the diagram, a massless string connects two blocks of mass 30 kg and 50 kg that are on a flat, frictionaless surface. A force pulls on the 50 kg block, as shown. If the force pulling on the 50 kg block is 100 N, what is the tension in the string connecting the two blocks?
Start by drawing in the forces acting on each block. You could also draw in the force of gravity and the normal force for each block, but they have been omitted from the image because they cancel each other out for each block and because there is no friction in this problem.
We are given in the question that the force is 100 N. Since the blocks are connected by a string, they will therefore accelerate at the same rate, and we can treat them as a system that moves as if it were one object of total mass 80 kg (30 kg plus 50 kg). Use Newton's second law:
In this problem, the two tension forces form an action/reaction pair and therefore are equal in magnitude but opposite in direction (Newton's third law). So:
We can solve for acceleration, since the tensions cancel out.
Now that we have acceleration, we need to write a new equation in which the tension force does not cancel out so that we can solve for the tension .
Do this by using Newton's second law again, except for only one of the blocks:
Lets consider the 30 kg block. The only force acting on the 30 kg block is the tension , and the acceleration is what we found above.
Example Question #311 : Forces
A ball with mass is on a ramp as illustrated below:
Find the magnitude of the ball's normal force.
The normal force is perpendicular to the plane:
First, we need to find .
We can solve for using the trigonometric equation that applies in this instance. We know the length of the side opposite of (5 m) and the length of the side adjacent to (10 m), so we can use the following equation to solve for :
Rearranging to solve this equation for , you get
Substituting in the side lengths of the given triangle, we can solve for .
Note that the normal force is one of the legs of another right triangle. The other leg is the parallel force, and the hypotenuse is the force of gravity.
Using trigonometry, we know that
because , or, in terms of this problem, .
Substituting in the known values into this equation, we can solve for the normal force:
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