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Hi, everyone.
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In this video, we are going to take a look at rotational motion, and we're going to consider the earth as it moves around the sun.
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All right.
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So the period, the amount of time it takes the earth to go around the sun is 365 .25 days.
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So 365 .25 days.
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Okay.
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And so let's suppose we have a time of one day.
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And we want to find the rotation angle, how much the earth goes around.
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So if this is the orbital path and this is the sun, as for sun.
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So in one day's time, we want to find this delta theta, okay, that angle.
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And it takes 365 days to go all the way around.
01:01
Okay.
01:01
Well, the angular velocity omega is two -pile.
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Radians over the period t so two pi all the way around in the time it takes is the period t the total time for one to go around once and omega is also equal to delta theta over t so our rotation angle delta theta is omega times t all right so delta theta is two pie little t over big t okay delta theta is two pi times one day divided by 365 .2 days okay and so we crunch that out and get 1 .72 times 10 to the minus two radians okay now let's look at change in velocity and so try to do an accurate drawing here so now we want to find delta v what is l2b.
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Okay.
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So let's draw our picture again.
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So we have our circle.
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Here's an r.
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Here's an r.
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The circular path is s.
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That angle is delta theta.
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Okay.
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And the straight line between the two points, say a and b, is delta r.
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All right, so let's draw it again.
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So it's about there and there.
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This time we have, say, a v1 there and a v2 there.
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And we want the change in vs.
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All right, and this is still the same delta theta.
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Okay, so we'll draw v2 and then we'll draw minus v1 and we'll get delta v2 over here.
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So here is our v2 minus v1.
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It's just going in the opposite direction of this one.
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Okay, so it's hard to tell where theta is in that picture.
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So a lot of times we'll just draw v1 and then we'll draw v2 and we'll have our delta v.
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All right.
03:45
And so we also have, let's just draw the r triangle.
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We have the r, we have the r, and we have the delta r.
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Okay.
04:00
And so what we can do is say these are similar triangles because this is delta theta and this is delta theta.
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So we can say delta v is to v.
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Right, let me make that look more like a v.
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Delta v is to v as delta r is to, sorry, as, as, delta s is to r.
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So we can actually use the curve.
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We can use the curve too.
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So we can, we'll use this instead.
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We'll do the r.
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We'll do the r.
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And when it's a circular path, that's the s.
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So we'll say the delta s over to the r.
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All right.
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And then s is equal to r times delta s is r times delta theta.
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So let's scroll here.
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All right.
05:06
So let's substitute for delta s.
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So we've got delta v over v is r delta theta over r.
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So those r's are going to cancel...