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Question about Planetary orbit and satelites |
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| Apr13-11, 09:27 PM | #1 |
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Question about Planetary orbit and satelites
1. The pro blem statement, all variables and given/known data
the question: 9.0 × 10^3 kg satellite orbits the earth at the distance of 2.56 × 10^7 m from Earth’s surface. What is its period? They give me a multiple choice, but let's figure this out with out it. okay so my variables known are the mass of the satelite: "MSat"- 9.0*10^3 d/r= 2.56 × 10^7 m mearth: 5.9742 × 10^24 kilograms G= 6.67*10^-11 2. Relevant equations Kepler's Law (?) T^2= 2*pi*r(^3/2)/G*Mp 3. The attempt at a solution So for some reason I bet that equation is NOT correct. Ive been searching all over google and through my notes and its all i can come up with. I'm not sure if I use the mass of the satelite or the mass of earth in the equation. I dont understand why they would even give me the mass of the satelite if im not supposed to use it though so I put into my calculator: T=squrt: 2*(3.14)^2* 2.56 × 10^7 m (or is it the radius of earth+the distance given(?) / (6.67*10^-11)* 5.9742 × 10^24 or do i use the mass of satelite here? |
| Apr13-11, 09:35 PM | #2 |
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Your equation in #2 has a typo. It should be,
[tex] T^2 = \frac{4 \pi^2 r^3}{GM} [/tex] This is Kepler's Third Law, which may help with Googling. See if you can find what you are supposed to plug in for r and M on your own. One hint: |
| Apr13-11, 09:44 PM | #3 |
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well, when you put it like that...
:) |
| Apr13-11, 10:02 PM | #4 |
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Question about Planetary orbit and satelites
i used your equation. i used the satelite for mass. i tried the radius as the radius given AND the radius give+the radius of earth itself, neither time did i get an answer even close
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| Apr13-11, 10:06 PM | #5 |
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& the period of a satellite does NOT depend on its mass, so why in the world would they give me its mass?
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| Apr13-11, 10:10 PM | #6 |
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Let's figure out the radius first. Our two options are the height itself, or the height plus the planetary radius. Which one is right?
Hint: if there was no atmosphere, satellites could orbit at ground level (if there were no mountains, people, etc to get in their way). Which option makes sense in that context? |
| Apr13-11, 10:14 PM | #7 |
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option B
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| Apr13-11, 10:18 PM | #8 |
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using your equation:
(sqrt(4 * (pi^2)) * (2.56 * (10^7))) + (((6 378.1^3) / (6.67 * (10^11))) * (5.9742 * (10^24))) = 2.32395597 × 10^24 all of my options' powers of ten are 4. i dont see how/where I am going wrong. Using the mass as the satellites mass (sqrt(4 * (pi^2)) * (2.56 * (10^7))) + (((6 378.1^3) / (6.67 * (10^11))) * (9 * (10^3))) = 160 853 045 <---wrong as well. hmm.:/ |
| Apr13-11, 10:22 PM | #9 |
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Yup. And that's a general result; outside of a spherical body, the gravitational force from that body is the same as if all the mass was concentrated at the center. So in this kind of problem, r always means "distance from the center."
Now for the mass. Why did they give you both masses? To make you think about this question! If you're still stuck, drop a textbook* and a pencil from the same height and see which one falls faster. *Not a physics book. Drop a math or chemistry book, that's all they're good for. ![]() Edit: Looks like you have an order-of-operations error. Slow down and make sure you're putting the numbers into the calculator correctly. |
| Apr13-11, 10:27 PM | #10 |
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okay, okay. i see. So why arent my 'generally correct' results = any of my choices?
by the way, they hit the ground at precisely the same time. |
| Apr13-11, 10:35 PM | #11 |
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(Also, I checked the answer and got [something] times 104 seconds. So it does work out.) |
| Apr13-11, 10:43 PM | #12 |
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no it does not. just how far it is away from the mcenter, i suppose.
:) well thank you for the help |
| Apr13-11, 10:47 PM | #13 |
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I think you might just be making calculator errors. Can you show me what you're entering in?
Two things: 1. Make sure you are really dividing by the denominator. 2. The equation above has T^2 on the LHS. So you have to take the square root at the end to get T. |
| Apr13-11, 11:05 PM | #14 |
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i using those equations from above.
along with endless variations of it. including an equation of velocity, (v=sqrt(G*m^2)/R, as in distance from center, like you said. then inserting value of v into T=2piR/V which is a random equation I found in my notes. im so lost. |
| Apr13-11, 11:05 PM | #15 |
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what you're saying makes sence, i just dont get how to apply it.
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| Apr14-11, 12:21 AM | #16 |
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Those two equations are actually how you derive my equation at the top. So let's look at those. It's a good idea to know how equations are related. So, we have:
Fg = GMm/r2 Where F is the force of gravity, G is the gravitational constant, M is the mass of the planet, m is the mass of the satellite, and r is the distance between the satellite and the center of the planet. This is the fundamental equation that describes gravity. Now, imagine a particle moving in a circle. You have to exert a force to keep it moving in a circle, otherwise it flies off in a straight line. That force is, Fcircle = mv2/r For a satellite, gravity is the force that keeps the satellite moving in a circle. So we should set the two forces equal to get, mv2/r = GMm/r2 We can divide both sides by m to get and multiply both sides by r to get, v2 = GM/r (Notice the mass of the satellite is gone, as expected). Okay, now to introduce the orbital period. The circumference of a circle is: [tex] c = 2 \pi r [/tex] And speed v is distance divided by time. The time it takes to complete on circle is T, by definition. So we have, [tex] v = c/T = 2 \pi r/T [/tex] Okay, so as a first step, plug the last equation into v in the fourth equation, and show that the result is, [tex] T^2 = \frac{4 \pi^2 r^3}{GM} [/tex] Which is the equation from before. |
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| kepler's 3rd law, newton, orbit, planets, satellite |
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