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What is the minimum energy required to launch a satellite of mass \(m\) from the surface of a planet of mass \(M\) and radius \(R\) in a circular orbit at an altitude of \(2 R ? (a) \)\frac{5 \mathrm{GmM}}{6 R}\( (b) \)\frac{2 G m M}{3 R}\( (c) \)\frac{G m M}{2 R}\( (d) \)\frac{G m M}{3 R}$

Short Answer

Expert verified
The minimum energy required is \(\frac{5GmM}{6R}\). Option (a).

Step by step solution

01

Assess the Satellite's Total Energy

To launch the satellite in a stable circular orbit at an altitude of \(2R\), we need to calculate the satellite's total mechanical energy: kinetic plus potential energy. At an altitude of \(2R\), the height from the planet's center is \(3R\) (since \(R + 2R = 3R\)).
02

Calculate Gravitational Potential Energy

The gravitational potential energy \(U\) at a distance \(r = 3R\) from the center of the planet is given by the formula \(U = -\frac{GmM}{r}\). Substituting the value, we get \(U = -\frac{GmM}{3R}\).
03

Calculate Kinetic Energy for Circular Orbit

For a stable circular orbit, the gravitational force provides the centripetal force: \(\frac{GmM}{(3R)^2} = \frac{mv^2}{3R}\). Solving for \(v\), we find \(v = \sqrt{\frac{GM}{3R}}\). Thus, the kinetic energy \(K\) is \(K = \frac{1}{2}mv^2 = \frac{1}{2}m\left(\sqrt{\frac{GM}{3R}}\right)^2 = \frac{GmM}{6R}\).
04

Determine Satellite's Total Orbital Energy

The total energy \(E\) of the satellite in orbit is the sum of potential and kinetic energy: \(E = K + U = \frac{GmM}{6R} - \frac{GmM}{3R}\). Simplifying gives \(E = -\frac{GmM}{6R}\).
05

Calculate Initial and Final Energies to Determine Energy Required

Initially, on the surface, the satellite's potential energy is \(-\frac{GmM}{R}\) and kinetic energy is zero. Therefore, initial energy \(E_i = -\frac{GmM}{R}\). Final energy \(E_f\) is total orbital energy \(-\frac{GmM}{6R}\). The energy required is \(E_f - E_i = \left(-\frac{GmM}{6R}\right) - \left(-\frac{GmM}{R}\right) = \frac{5GmM}{6R}\).
06

Conclusion

The minimum energy required to launch the satellite into the specified orbit is \(\frac{5GmM}{6R}\). This matches option (a).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Gravitational Potential Energy
Gravitational potential energy is an essential concept in physics, particularly when dealing with orbital mechanics. When a satellite is located at a certain distance from a massive planet, it possesses gravitational potential energy due to the gravitational attraction between the two bodies. This energy depends on the masses of both the satellite and the planet, as well as the distance between them.
For a satellite at a distance of 3R from the center of the planet, the gravitational potential energy (U) is calculated using the formula:
  • \( U = -\frac{GmM}{r} \)
G represents the gravitational constant, m is the satellite's mass, M is the planet's mass, and r is the distance from the planet's center. At an altitude of 2R from the planet's surface, r becomes 3R because you add the planet's radius (R) to the altitude (2R).This potential energy is negative, which reflects that work must be done against the planet's gravitational pull to bring the satellite further from the surface.
Kinetic Energy for Circular Orbits
Kinetic energy is the energy of motion, and it plays a critical role in keeping a satellite in a stable circular orbit. For an object in a circular orbit, its speed must be such that the gravitational force acts as the centripetal force needed to maintain the orbit.
To find the orbital speed \( v \) of a satellite in a circular orbit of radius 3R, we use the balance between gravitational and centripetal force:
  • \( \frac{GmM}{(3R)^2} = \frac{mv^2}{3R} \)
Solving for \( v \), we find:
  • \( v = \sqrt{\frac{GM}{3R}} \)
Using this speed, the kinetic energy \( K \) of the satellite can be calculated as:
  • \( K = \frac{1}{2}mv^2 = \frac{GmM}{6R} \)
This expression illustrates how kinetic energy in circular orbits is derived from balancing gravitational attraction with the need to maintain a stable orbital path.
Orbital Mechanics
Orbital mechanics is the study of how objects move in space under the influence of gravity. Central to this field is understanding how satellites or planets follow paths around massive bodies, guided by gravitational forces.
When placing a satellite in orbit, it’s important to know what altitude and speed are necessary to achieve a stable, circular path. The essence of achieving such orbits lies in correctly calculating both the potential and kinetic energy required at the intended orbital radius.
High altitudes require careful calculations to ensure the satellite has enough speed to stay in orbit without it being too high to escape or too low to crash back to the planet’s surface. The principles of conservation of energy and angular momentum help predict these orbital paths.
This field not only assists in earth-based satellite deployments but is crucial for interplanetary missions, space explorations, and ensuring that space stations and payloads remain in their intended orbits.
Energy Calculations in Physics
Energy calculations are fundamental in physics, especially when analyzing systems involving motion and forces, such as launching satellites. These calculations help determine the work needed to move a satellite from its initial position on a planet's surface to a specific altitude in space.
Calculating the minimum energy to launch a satellite involves:
  • Determining initial and final gravitational potential energies.
  • Assessing initial and final kinetic energies.
  • Finding the difference between these total initial and final energies to obtain the energy required.
In the exercise, the initial total energy includes potential energy at the surface with no initial kinetic energy, while the final energy incorporates both potential and kinetic energies in orbit. The energy needed is therefore the additional energy required to move the satellite into its desired orbit.
These calculations ensure the satellite receives the right amount of energy to achieve and maintain its orbit, minimizing fuel use and optimizing launch design.

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