1. **Using Gravitational Force and Centripetal Force:**
For a satellite of mass m orbiting Earth at height h above the surface, the gravitational force provides the required centripetal force:
GMm / (R + h)² = mv² / (R + h).
Simplifying, we get:
GM / (R + h) = v². (1)
2. **Relate Orbital Velocity to Period:**
The orbital velocity v can also be expressed in terms of the orbital period T:
v = 2π(R + h) / T. (2)
3. **Equate Gravitational Force with Centripetal Acceleration:**
We know that GM = gR² (where g is the acceleration due to gravity on Earth's surface). Substituting this in equation (1):
gR² / (R + h) = v².
4. **Combine Equations (1) and (2):**
Substitute v from equation (2) into the above expression:
gR² / (R + h) = (2π(R + h) / T)².
Rearranging gives:
T²R²g / (2π)² = (R + h)³.
5. **Solve for Height h:**
Taking the cube root of both sides, we get:
R + h = (T²R²g / 4π²)^(1/3).
Therefore,
h = (T²R²g / 4π²)^(1/3) - R.
**Answer:** (T²R²g / 4π²)^(1/3) - R (Option 2)
If the distance of the earth from Sun is $15 \times 10^6 km$ Then the distance of an imaginary planet from Sun, if its period of revolution is $2.83$ years is :
The portion of the line \( 4x + 5y = 20 \) in the first quadrant is trisected by the lines \( L_1 \) and \( L_2 \) passing through the origin. The tangent of an angle between the lines \( L_1 \) and \( L_2 \) is: