Astrophysics - calculating orbital period

In summary, the conversation involved finding an approximation for a satellite in low-Earth orbit using the equation P = C(1 + 3h/2R_E), where h is the height of the satellite, C is a constant, and R_E is the radius of the earth. The suggested approach was to use centripetal acceleration and Newton's gravitational law, with a hint to rewrite the acceleration as ω2r and compare r with r+h.
  • #1
superdave
150
3

Homework Statement


Show that a satellite in low-Earth orbit is approximately P = C(1 + 3h/2R_E) where h is the height of the satellite, C is a constant, and R_E is the radius of the earth)

Homework Equations



Unsure

The Attempt at a Solution



I have no idea how to approach this.
 
Last edited:
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  • #2
hi superdave! :smile:

(try using the X2 icon just above the Reply box :wink:)

use centripetal acceleration and Newton's gravtiational law …

what do you get? :smile:
 
  • #3
a= GM/r2 =v2/r

v2=GM/r

Aaand, I'm stuck again.
 
  • #4
hi superdave! :smile:

(just got up :zzz: …)

hint: you need P, so write the centripetal acceleration as ω2r instead of v2/r :wink:

(and then compare r with r+h)
 
  • #5


As an astrophysicist, I can offer some guidance on how to approach this problem. First, we need to understand the concept of orbital period, which is the time it takes for a satellite to complete one full orbit around a celestial body, in this case, the Earth. This can be calculated using Kepler's Third Law, which states that the square of the orbital period (P) is proportional to the cube of the semi-major axis (a) of the orbit. In this case, the semi-major axis is equal to the sum of the Earth's radius (R_E) and the height of the satellite (h).

Next, we can use the equation for the semi-major axis (a) of an orbit, which is a = (r_1 + r_2)/2, where r_1 is the distance from the center of the Earth to the satellite and r_2 is the distance from the satellite to the edge of the Earth's atmosphere. Since the satellite is in low-Earth orbit, we can assume that r_2 is approximately equal to the Earth's radius (R_E).

Therefore, the semi-major axis (a) can be written as a = (R_E + h)/2. Plugging this into Kepler's Third Law, we get P^2 = (R_E + h)^3, where P is the orbital period. Solving for P, we get P = C(1 + 3h/2R_E), where C is a constant. This shows that the orbital period is indeed approximately equal to C(1 + 3h/2R_E), as given in the homework statement.

In conclusion, the orbital period of a satellite in low-Earth orbit can be calculated using Kepler's Third Law and the equation for the semi-major axis of an orbit. This shows the relationship between the height of the satellite and the orbital period, as well as the importance of the Earth's radius in determining the orbital period.
 

1. What is an orbital period?

An orbital period is the time it takes for an object to make one complete orbit around another object.

2. How is the orbital period calculated?

The orbital period is calculated using Kepler's Third Law, which states that the square of the orbital period is directly proportional to the cube of the semi-major axis of the orbit.

3. What is the semi-major axis?

The semi-major axis is the longest radius of an elliptical orbit, extending from the center of the orbit to the farthest point from the center.

4. Can the orbital period change?

Yes, the orbital period can change due to factors such as gravitational interactions with other objects, changes in the shape of the orbit, or changes in the mass of the objects involved.

5. What are some real-world applications of calculating orbital period?

Calculating orbital period is essential in understanding and predicting the movements of celestial bodies, such as planets, moons, and comets. It is also crucial in space exploration and satellite missions, as it helps determine the optimal orbit for spacecraft and satellites.

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