Satellites play a crucial role in modern life, enabling everything from global communication to weather forecasting. Two primary types of satellites are geostationary and polar satellites, each serving distinct purposes. Geostationary satellites remain fixed above a specific point on Earth, orbiting at the same rotational speed as the planet. This allows them to provide continuous coverage over a large area, making them essential for broadcasting, GPS, and meteorology. On the other hand, polar satellites orbit the Earth from pole to pole, covering the entire surface over time. They are invaluable for environmental monitoring and scientific research, capturing high-resolution images of every part of the globe. Just like surveillance cameras watching over specific locations or drones flying over large areas to gather data, these satellites help us stay connected and informed about global events and natural phenomena.
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A satellite which appears stationary relative to the Earth is called a geostationary or geosynchronous satellite.
A geostationary satellite will stay the same place above the earth always, such a satellite is never at rest. Geostationary satellites appear stationary due to their zero relative velocity with respect to their place on Earth.
It is also known as parking orbit.
Now, you can say that the time period of the geostationary satellite is also 24 hours or 86400 sec.
So $\mathrm{T}=24$ hours or 86400 sec.
and we know that the Height of the Satellite is given by
$
h=\left(\frac{T^2 g R^2}{4 \pi^2}\right)^{\frac{1}{3}}-R
$
So putting $\mathrm{T}=24$ hours or 86400 sec.
We get the height of geostationary satellite from the surface of the earth
$
\text { as } h=6 R=36000 \mathrm{~km}
$
Its sense of rotation should be the same as that of Earth about its own axis. l.e., in an anti-clockwise direction (from west to east).
A geostationary satellite is used for telecommunication, weather forecasting, etc.
A polar satellite is a satellite whose orbit is perpendicular or at right angles to the equator. or in simple words, it passes over the north and south poles as it orbits the earth. It can also be used as a communication satellite for countries/areas near the poles where Geostationary satellites have no / Poor coverage.
Example 1: Which one of the following statements regarding geostationary satellites of the earth is incorrect?
1) It should revolve in an orbit concentric and coplanar with the equatorial plane
2) The time period of revolution is 16 hours.
3) The height of the geostationary satellite from the centre of the earth is 42400km.
4) The orbital velocity of a geostationary satellite is 3.08km/s.
Solution:
geostationary satellite
Satellites that appear stationary relative to Earth are geostationary satellites, also known as communication satellites or geosynchronous satellites
The period of revolution is the same as the revolution of the earth, T = 24hrs.
The height of a geostationary satellite from the earth's centre is 4200km. and the Orbital velocity of a geostationary satellite is 3.08km/s.
Hence, the answer is the option (2)
Example 2: A geostationary satellite has always to be at an altitude of (in kilometres) :
1) 36000
2) 24000
3) 30000
4) 20000
Solution:
As we know, the time period
Geostationary and polar satellites are given by
$
T=2 \pi \sqrt{\frac{r^3}{G M}}=2 \pi \sqrt{\frac{(R+h)^3}{g R^2}}
$
By squaring and rearranging both sides
$
\begin{aligned}
& \frac{g R^2 T^2}{4 \pi^2}=(R+h)^3 \\
\Rightarrow & h=\left(\frac{T^2 g R^2}{4 \pi^2}\right)^{1 / 3}-R
\end{aligned}
$
So, put the value, $T=24 h=24 \times 60 \times 60=86400 s$
$
\begin{aligned}
& R=\text { Radius of the earth }=6400 \mathrm{~km} \\
& g=9.8 \times 10^{-3} \mathrm{~km} / \mathrm{s}^2
\end{aligned}
$
Substituting these values in the equation of the formula of height, we get-
$
h=(42400-6400) \mathrm{km}=36000 \mathrm{~km}
$
Hence, the answer is the option (1).
Example 3: Given the radius of earth ‘R’ and the length of a day ‘T’, the height of a geostationary satellite is [G = gravitational constant, M = mass of the earth]
1) $\left(\frac{4 \pi^2 G M}{T^2}\right)^{\frac{1}{3}}$
2) $\left(\frac{4 \pi G M}{T^2}\right)^{\frac{1}{3}}-R$
3) $\left(\frac{G M T^2}{4 \pi^2}\right)^{\frac{1}{3}}-R$
4) $\left(\frac{G M T^2}{4 \pi^2}\right)+R$
Solution:
The height of geostationary satellites from the surface of the Earth is $h=6 R=36000 \mathrm{Km}$
$
\begin{aligned}
T & =2 \pi \sqrt{\frac{r^3}{G M}} \\
T & =2 \pi \sqrt{\frac{(r+h)^3}{G M}} \\
h & =\left(\frac{G M T^2}{4 \pi^2}\right)^{\frac{1}{3}}-R
\end{aligned}
$
Hence, the answer is the option (3).
Example 4: A satellite of mass M is in a circular orbit of radius R about the centre of the Earth. A meteorite of the same mass, falling towards the earth, collides with the satellite completely inelastically. The speeds of the satellite and the meteorite are the same, just before the collision. The subsequent motion of the combined body will be :
1) in an elliptical orbit
2) such that it escapes to infinity
3) in a circular orbit of a different radius
4) in the same circular orbit of radius R
Solution:
The shape of the orbit of the satellite
If $V<V_o$, then the satellite does not remain in its circular path rather it traces a spiral path and falls on the earth
$
V=V_e
$
satellite move along a parabolic path
wherein
$
V=V_o
$
Satellite revolves in a circular path
$
V>V_e
$
Satellite will move along a hyperbolic path
Apply momentum conservation
$\begin{aligned} & m V \hat{l}-m V \hat{j}=2 m \rightarrow \overrightarrow{V_2} \\ & V_2=\frac{1}{2} \times \sqrt{2} V_0=\frac{V_0}{2} \\ & \text { So }_2<V_0<\sqrt{\frac{G M}{R}}\end{aligned}$
So it will move in an elliptical orbit
Hence, the answer is the option (1).
Geostationary satellites orbit at 36,000 km above Earth, remaining fixed over one location, making them ideal for continuous communication, broadcasting, and weather monitoring. Polar satellites, however, orbit from pole to pole, covering the entire globe and providing crucial data for environmental monitoring and scientific research. Both satellite types play vital roles in connecting and informing us about global events and natural phenomena.
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