Problem 768
Question
A small satellite is revolving near earth's surface. Its orbital velocity will be nearly \(=\ldots \ldots \ldots \ldots \mathrm{kms}^{-1}\). (A) 8 (B) 4 (C) 6 (D) \(11.2\)
Step-by-Step Solution
Verified Answer
The orbital velocity of a small satellite revolving near the Earth's surface is approximately 8 \(\mathrm{km/s}\).
1Step 1: Write the formula for orbital velocity
Orbital velocity (V) is the velocity an object requires to stay in a stable orbit around another celestial body, like a planet or a moon. The formula for orbital velocity is given by:
\[V = \sqrt{\frac{GM}{R}}\]
Where:
- V is the orbital velocity
- G is the gravitational constant (\(6.67 \times 10^{-11} \mathrm{N} \cdot \mathrm{m}^2 \cdot \mathrm{kg}^{-2}\))
- M is the mass of the celestial body (in this case, Earth's mass, which is \(5.97 \times 10^{24} \mathrm{kg}\))
- R is the distance from the center of the celestial body to the object in orbit (in this case, Earth's radius, which is approximately \(6.37 \times 10^6 \mathrm{m}\))
2Step 2: Substitute values and calculate the orbital velocity
We'll now substitute the given values for G, M, and R into the orbital velocity formula:
\[V = \sqrt{\frac{(6.67 \times 10^{-11} \mathrm{N} \cdot \mathrm{m}^2 \cdot \mathrm{kg}^{-2})(5.97 \times 10^{24} \mathrm{kg})}{(6.37 \times 10^6 \mathrm{m})}}\]
Now we'll solve for V:
\[V \approx 7.9 \times 10^3 \mathrm{m/s}\]
3Step 3: Convert the orbital velocity to \(\mathrm{km/s}\) and select the correct answer
Wrap up the process by converting the orbital velocity from \(\mathrm{m/s}\) to \(\mathrm{km/s}\) as requested:
\[V \approx 7.9 \times 10^3 \mathrm{m/s} \times (\frac{1 \mathrm{km}}{1000 \mathrm{m}}) \approx 7.9 \mathrm{km/s}\]
Looking at the given choices, the closest option to our calculated orbital velocity of \(7.9 \mathrm{km/s}\) is choice (A) 8 \(\mathrm{km/s}\). So, the correct answer is:
(A) 8 \(\mathrm{km/s}\)
Key Concepts
Gravitational ConstantMass of EarthRadius of EarthSatellite Motion
Gravitational Constant
The gravitational constant, often represented by the symbol \( G \), plays a crucial role in calculations involving gravity, especially in celestial mechanics. It is a proportionality factor used in Newton's Law of Universal Gravitation, which describes the attractive force between two masses.
- The value of the gravitational constant is \( 6.67 \times 10^{-11} \mathrm{N} \cdot \mathrm{m}^2 \cdot \mathrm{kg}^{-2} \).
- This value is tiny, reflective of the feeble nature of gravitational force compared to other fundamental forces.
- \( G \) is used universally, providing a consistent measure that helps us understand the gravitational effects in cosmic scale calculations.
Mass of Earth
The mass of Earth is a critical parameter when calculating the orbital velocity of a satellite. It represents the total mass of our planet and is a central component in the formula governing gravitational forces between the Earth and any object in its vicinity.
- Earth’s mass is approximately \( 5.97 \times 10^{24} \mathrm{kg} \).
- This huge mass contributes significantly to its gravitational pull, affecting both natural satellites and human-made ones.
- Understanding Earth's mass helps scientists and engineers to determine the capabilities and limits of satellite motion.
Radius of Earth
The radius of Earth is a vital dimension in the formula for orbital velocity. It is the average distance from Earth's center to its surface and helps determine the gravitational field strength experienced by an object in orbit.
- The average radius of Earth is approximately \( 6.37 \times 10^6 \mathrm{m} \) or \( 6,370 \ \mathrm{km} \).
- This measurement is key to calculating the orbital path and speed necessary to maintain orbit close to Earth's surface.
- When a satellite orbits at this altitude, it benefits from a balance between gravitational pull and the centrifugal force due to its velocity.
Satellite Motion
Satellite motion refers to how satellites move in space, particularly around larger celestial bodies like Earth. These movements are governed by the principles of orbital mechanics and are influenced by gravitational forces.
- To remain in orbit, a satellite must travel at a precise speed, known as orbital velocity, which ensures the gravitational pull from the Earth is perfectly balanced by the satellite's inertia.
- If the velocity is too low, the satellite will fall back to Earth; if it's too high, it will escape into space.
- An orbital velocity near Earth’s surface is approximately \( 7.9 \ \mathrm{km/s} \), allowing satellites to stay aloft while orbiting in a stable path.
Other exercises in this chapter
Problem 766
The period of a satellite in circular orbit around a planet is independent of (A) the mass of the planet (B) the radius of the planet (C) mass of the satellite
View solution Problem 767
Two satellites \(\mathrm{A}\) and \(\mathrm{B}\) go round a planet \(\mathrm{p}\) in circular orbits having radii \(4 \mathrm{R}\) and \(\mathrm{R}\) respective
View solution Problem 769
A satellite revolves around the earth in an elliptical orbit. Its speed (A) is the same at all points in the orbit (B) is greatest when it is closest to the ear
View solution Problem 770
If the height of a satellite from the earth is negligible in comparison of the radius of the earth \(\mathrm{R}\), the orbital velocity of the satellite is (A)
View solution