00:01
So for this question, we are given a two -dimensional force field.
00:05
And we are given a path, which i'm labeling as c, which is y equals x cubed from the origin to the 0 .28.
00:13
So we're going to ask a couple of questions about this field.
00:16
The first is that we're going to calculate the work done by a particle traveling along this path.
00:23
So the work is going to be defined as the line integral of our force field, where c is our path.
00:34
So in order for us to do this, we're going to need a parametrization for this curve.
00:40
And whenever you have a function given in two variables, i recommend the nicest parametrization is to let your independent variable x be your parameter t.
00:54
And then we get this y component really nicely, which will be our t cubed.
01:01
And when you do a line integral of a vector field, you need the derivative of your parametrization.
01:07
So in this case, we should get the 1 and 3t squared.
01:13
So we now have a single integral, an ordinary one, where now we need to have bounds in terms of t.
01:27
So what's nice about the way we have it set up is because since our x component is t, we get that our bounds are going to be shown in the initial and endpoints.
01:39
So from 0 to 2 will be where we take our integral.
01:43
We'll have our vector field.
01:45
And we need to evaluate the vector field at our parametrization.
01:52
So we have the x and y components.
01:54
These will get substituted in to our field f.
01:57
So we have x times y, which will be t to the fourth.
02:01
And then we have 2y, which would be 2t cubed.
02:09
And this will now be dotted with the derivative, which we calculated already.
02:17
And there we go.
02:21
So now let's go ahead and evaluate the dot product.
02:28
You should get t to the fourth plus 6t to the fifth.
02:39
Great.
02:39
So now we have our single integral.
02:41
And we can calculate the work.
02:43
So we get 1 fifth t to the fifth plus t to the sixth from 0 to 2.
02:54
And substitute in your 2, you will get 32 over 5 plus 64...