Orbital Velocity
Orbital Velocity: Orbital
velocity is that velocity required to put the satellite into its orbit around
the earth.
Expression for Orbital Velocity:
Let
M = mass
of the earth,
R = radius of
the earth,
m
= mass of the satellite,
= orbital velocity of the satellite
h = height of
the satellite above the earth surface
R
+ h = orbital radius of the
satellite,
According
to the law of gravitation the force of the gravity on the satellite is
F
=
The
centripetal force required by the satellite to keep it in its orbit is
F
=
In
equilibrium, the centripetal force is just provided by the gravitational pull
of the earth, so
=
=
∴ Orbital
velocity,
= ------
(i)
If
g is the acceleration due to gravity
on the earth surface then
g
=
GM
=
Hence
=
=
When the satellite
revolves close to the surface of the earth h
= 0 and orbital velocity will become
=
As g
= 9.8 ms−2 and R =
6.4 × 106 m, so
=
= 7.92
× 103 ms−1
= 7.92
kms−1
Relation between Orbital Velocity and Escape Velocity:
The
escape velocity of a body from the earth’s surface is
=
The
orbital velocity of a satellite revolving close to the earth’s surface is
=
∴ =
=
or =
Hence the escape velocity of a body from the
earth’s surface is times
its velocity in a circular orbit just above the earth’s surface.
Problems:
1. The
orbit of a geostationary satellite is concentric and coplanar with the equator
of earth and rotates along the direction of rotation of earth. Calculate the
height and speed. Take mass of earth = 5.98 ×
1027 g and its radius = 6400 km. given = 9.87.
Solution:
Here T = 24 × 3600 s,
G = 6.67 ×
10−11
Nm2kg−2
M = 5.98 ×
1027
g = 5.98 ×
1024 kg
R = 6400 km
R + h =
=
= 4.225 × 107 m
= 42250 km
∴ h
= 42250 − 6400
= 35850 km
Orbital speed,
=
=
=
3.071 kms−1
2. An artificial satellite
of mass 100 kg is in a circular orbit of 500 km above the earth surface. Take radius
of earth as 6.5 × 106 m. (i) Find the acceleration due to gravity at any point along the
satellite path. (ii) What is the centripetal acceleration of satellite? Take g = 9.8 ms−2
Solution:
Here h
= 500 km
=
0.5 × 106 m
R = 6.5 ×
106 m
∴ R + h = 7.0 × 106 m
(i) g’ = g
= 9.8
= 8.45 ms−2
(ii) ac =
= ×
= 8.45 ms−2
3. A space ship is launched
into a circular orbit close to the earth’s surface. What additional velocity
has now to be imparted to the space ship in the orbit to overcome the
gravitational pull? (Radius of the earth = 6400 km, g = 9.8 ms−2).
Solution:
Orbital velocity near the earth surface,
=
Escape velocity,
=
=
Additional velocity required
=
=
= 0.414 ×
= 3.278 × 103 ms−1
=3.278 kms−1
4. An artificial satellite revolves around the
earth at a height of 1000km.The radius of the earth is 6.38 × 103
km. Mass of the earth is 6 × 1024 kg and G = 6.67 × 10−11 Nm2 kg−2.
Find its orbital velocity and period of revolution.
Solution:
Here
h = 1000 km
= 106
m
R =
6.38 × 103 km
=
6.38 × 106 m
∴ R
+ h = 7.38 × 106 m,
M = 6 × 1024
kg
Orbital
velocity
=
=
= 7364 ms−1
Period
of revolution,
T =
=
=
6297 s
5. An
remote sensing satellite of the earth revolves in a circular orbit at a height
of 250 km above the earth’s surface. What is the (i)
orbital speed and (ii) period of revolution of the satellite? Radius of the
earth, R = 6.38 × 106 m,
and acceleration due to gravity on the surface of the earth, g = 9.8 ms−2.
Solution:
(i) Here g = 9.8 ms−2, R = 6.38 × 106 m, h = 250,000 m
R + h =
6.38 × 106 + 250,000
= 6.63 × 106 m
The
orbital speed is given by
=
=
= 7.76 × 103 ms−1
=
7.76 kms−1
(ii)
The period of revolution of the satellite will be
T
=
=
=
5370 s
6. An artificial satellite is going round the
earth, close to its surface. What is the time taken by it to complete one
round? Given radius of earth = 6400 km.
Solution:
Here
R
= 6400 km = 6.4 × 106 m,
g
= 9.8 ms-2
Orbital
velocity near the earth surface is
=
=
=
7290 ms-1
Time
period,
T
=
=
=
5079 s
=
1.411 hour
7. A satellite revolves in an orbit close to the
surface of a planet of mean density 5.51 × 103 kg m−3.
Calculate the time period of satellite. Given G =
6.67 × 10−11
Solution:
Here
= 5.51 × 103 kgm−3
G
= 6.67 × 10−11 Nm−2 kg−2
Time
period of the satellite near the surface of the planet (h = 0) is
T
=
=
=
5062.7 s
8. An earth’s satellite makes a circle
around the earth in 90 minutes. Calculate the height of the satellite above the
earth surface. Given radius of the earth is 6400 km
and g = 980 cm−2.
Solution:
Here
T
= 90 minutes
= 5400s,
R
= 6400 km
= 6.4 ×
106 m
g
= 980 cm-2
= 9.8 ms-2
As T = 2π
∴ R + h =
=
=
6.668 × 106 m
= 6668 km
Hence h
= 6668 – R
= 6668 – 6400
= 268 km
9. If the period of revolution of
artificial satellite just above the earth surface T and the density of the earth be ,
then prove that is a universal constant. Also calculate the
value of this constant.
Solution:
As
T = 2π
=
M
=
For
the satellite revolving just above the earth’s surface, h = 0. So
M
=
Also,
M
=
∴ =
∴ = , which is
a universal constant
And =
= 1.41 × 1011 kgs2 m−3
10. In a
two stage launch of a satellite the first stage brings the satellite to a height
of 150 km and second stage gives it the necessary critical speed to put it in a
circular orbit around the earth. Which stage requires more expenditure of fuel?
(neglect due to air resistance, especially in the
first stage). Mass of the earth = 6.0 × 1024 kg, radius = 6400 km, G = 6.67 × 10−11 Nm2
kg−2.
Solution:
Work
done on the satellite in first stage,
W1
= P.E. at height of 150 km – P.E. at the surface of the earth
=
=
GMm
=
Work
done on the satellite in second stage,
W2
= energy required to give its orbital velocity
=
=
=
=
=
=
As
W2 > W1, so the second stage
requires more expenditure of fuel.