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  • Hi. It’s Mr. Andersen and this is AP Physics essentials video 51. It is on the work energy

  • principle. But before we get to that we should define both work and energy. What is energy?

  • Energy is the ability to do work. That does not help much. What is the energy we are going

  • to be talking about in this video? It is going to be kinetic energy. So that is energy due

  • to motion. And to figure that out remember it is one-half mv squared, where m is the

  • mass and v is the velocity of the object. If the object is bigger, if it is faster it

  • is going to have more kinetic energy. Now what is work? Work is simply a force times

  • a distance. So applying a force for a given amount of distance.

  • And so what is neat is that these two are equivalent. They are always going to be equal.

  • And so if you need to calculate the kinetic energy, a really good way to do it is to simply

  • calculate the work. And so if we are looking at baseball as it is moving it clearly has

  • kinetic energy. Where did it come from? It came from work of the pitcher. So the pitcher

  • is applying a force to that baseball over a given distance. And the amount of that work

  • is going to be equivalent to the amount of energy that is given to that baseball. And

  • so there is a equivalence between these two. So let’s start with work. So let’s say

  • we are applying a force to this object right here. So we are going to apply a constant

  • force to the right. And then we are going to move it a given distance. So watch what

  • happens. You can see it started at rest and it is accelerating. I just stopped the simulation

  • right here. And so we applied a constant force over a given distance. And so we did work.

  • Now what is neat is that is equivalent to the amount of energy that was given to that

  • object. This object now has kinetic energy. Now if we wanted to figure out that kinetic

  • energy we could break it down into the final kinetic energy, which is one half mv squared

  • minus the initial kinetic energy. But what is neat is if we just know the force and the

  • distance we have already figured out the amount of kinetic energy that is being added. Now

  • let’s work qualitatively for a second. Have we added energy to that object or have we

  • taken it away? Well since we applied a force to the right over a given distance we know

  • that the work is going to be a positive value. How else could we figure this out? Well if

  • we look at its initial kinetic energy, since it had a velocity of zero then we know that

  • this is a zero value. And if we are taking a value of a velocity minus a zero value we

  • know this is going to be a positive value. And so you can look at either the force and

  • where the force is being added over time. Or the change in the velocity and that is

  • going to tell you is energy being added or is it being taken away. Let’s look at a

  • different scenario. Now we have an object that is moving towards the right, and so when

  • I start it is going to be moving towards the right. Well let’s say we are applying a

  • net force to the left. What is going to happen here? You can see it is going to slow down.

  • And so what is happening to the amount of work? Well we have a negative force times

  • a distance and so we are decreasing the amount of kinetic energy in that object. We are taking

  • that energy away, which makes sense because the object is coming to rest. If we wanted

  • to look at the velocities we could see now that we have a final velocity of zero, so

  • this is a zero value right here, minus that initial velocity, and so you can see that

  • we are going to have a negative energy. We have lost energy. We have lost kinetic energy.

  • Now it is not as simple as that because sometimes you are going to apply a force and it is not

  • going to be in the same direction as the motion. And so let’s say we are pulling on that

  • object. So you could say we have a rope tied on to it. And we are moving it in that direction.

  • Okay. Now since we have moved it in that direction we have to breakdown that force vector into

  • its two component vectors. We have this, we will call that the force parallel. So it is

  • in the direction of the motion. And then we have this which is going to be the force perpendicular.

  • Now what is interesting is that it is only this force that is acting in the direction

  • of that motion. And therefore it is only that force that is doing work. The other force

  • is not doing any work since the motion is not in that direction. And so lots of times

  • when you are solving problems it is not as simple as figuring out the work. You have

  • to break that force down into its component force. And I will show you an example of that.

  • And so let’s start simple. Let’s say we have a cart. And that cart is moving from

  • the left to the right. And we are applying a constant force of 7.1 newtons. So how would

  • you figure out the work on that cart? It is really simple. You just say work is equal

  • to the force parallel. Again it is going to be in the direction of that motion times the

  • distance. And since we are given a force of 7.1 newtons times the distance 0.18 meters

  • it is really simple to solve for that. So what is going to be our work? It is simply

  • going to be 1.3 joules. Now that is the amount of work that was done on the cart. What is

  • neat is it also shows us the amount of kinetic energy that was added to that cart. We do

  • not have to figure out the mass and the velocity and initial velocity. We know by the amount

  • of work being applied to it that that is going to tell us the amount of kinetic energy added.

  • Let’s look at a cart that is already moving towards the right. We are applying a net force

  • to the left. Watch what happens here. Again it is slowing down. So how do you figure out

  • the amount of work on that? Well again it is force parallel. In this case it is antiparallel.

  • It is in the opposite direction. And so we have to put that in as a negative value. And

  • so we are going to have negative 0.93 joules. In other words we are taking energy away.

  • We are doing negative work on that object. Now let’s move that force in a different

  • direction. This makes the problem a little bit harder. You can always pause the video

  • and try to work this out. But let’s say we are applying a 9.6 newton force in this

  • direction but it is 32 degrees up from parallel. And watch what happens to that object. So

  • it is moving in that direction. So if I want to figure out the amount of energy that is

  • added to that cart all I have to do is figure out the force, force parallel times the distance.

  • What makes this problem a little bit harder remember is that we have to target this, which

  • is going to be that force in the parallel direction. How do we do that? Well we just

  • use a little bit of trigonometry. Since you know this angle and you know the hypotenuse

  • we can figure out this adjacent. And so to figure out that it is simply going to be the

  • force times the distance times cosine of theta. What is cosine of theta? It is the cosine

  • of this angle right here. And so that is going to give me a force and I can always check

  • that. It should be a value that is going to be less than the hypotenuse or less than 9.6

  • newtons. So if I plug that in my calculator I can find the cosine of 32. And the cosine

  • of 32 is 0.848. So it is decreasing that amount of force. But it is the force that is actually

  • moving in the direction of that motion. And so now I just simply multiply all of those

  • values and I get 1.5 joules. Again I am solving for significant digits here. And so how much

  • work is done on the cart? 1.5 joules. How much energy has been added to the cart? 1.5

  • joules. And so you know there is that equivalence. The amount of work done on that cart is equal

  • to the amount of energy that that cart has gained, which is kinetic energy minus initial

  • energy. And so if you wanted to, if you were given the mass of the object you could plug

  • that in. Since that object is accelerating we could say that its initial velocity is

  • 0. And so you could figure out its final velocity. And so again, work and energy are going to

  • be equivalent. How did it get the energy? We applied a certain amount of force over

  • a given distance. And so did you learn to make predictions about the changes in kinetic

  • energy of an object? Again, if it is moving faster it is going to have a higher amount

  • of kinetic energy. Can you use the force and the velocity to just qualitatively figure

  • out are we adding energy or are we taking it away? And then finally can you figure out

  • the amount of work on an object and therefore the amount of energy that is being added to

  • the object? I hope so. And I hope that was helpful.

Hi. It’s Mr. Andersen and this is AP Physics essentials video 51. It is on the work energy

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B1 中級

工作能量原理 (Work Energy Principle)

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    Cheng-Hong Liu 發佈於 2021 年 01 月 14 日
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