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Page 1
GRAVITATION
THE DISCOVERY OF THE LAW OF GRAVITATION
The way the law of universal gravitation was discovered is often considered the paradigm
of modern scientific technique. The major steps involved were
? The hypothesis about planetary motion given by Nicolaus Copernicus (1473-
1543).
? The careful experimental measurements of the positions of the planets and the
Sun by Tycho Brahe (1546-1601).
? Analysis of the data and the formulation of empirical laws by Johannes Kepler
(1571-1630).
? The development of a general theory by Isaac Newton (1642-1727).
NEWTON'S LAW OF GRAVITATION
It states that everybody in the universe attracts every other body with a force that is
directly proportional to the product of their masses and is inversely proportional to the
square of the distance between them.
F?m
1
m
2
and F?
1
r
2
so F?
m
1
m
2
r
2
?F=-
Gm
1
m
2
r
2
r ˆ[G= Universal gravitational constant ]
{Note: This formula is only applicable for spherical symmetric masses or point masses.}
VECTOR FORM OF NEWTON'S LAW OF GRAVITATION:
Let ???
12
= Displacement vector from ?? 1
to ?? 2
r ?
21
= Displacement vector from m
2
to m
1
F
??
21
= Gravitational force exerted on m
2
by m
1
F
??
12
= Gravitational force exerted on m
1
by m
2
Page 2
GRAVITATION
THE DISCOVERY OF THE LAW OF GRAVITATION
The way the law of universal gravitation was discovered is often considered the paradigm
of modern scientific technique. The major steps involved were
? The hypothesis about planetary motion given by Nicolaus Copernicus (1473-
1543).
? The careful experimental measurements of the positions of the planets and the
Sun by Tycho Brahe (1546-1601).
? Analysis of the data and the formulation of empirical laws by Johannes Kepler
(1571-1630).
? The development of a general theory by Isaac Newton (1642-1727).
NEWTON'S LAW OF GRAVITATION
It states that everybody in the universe attracts every other body with a force that is
directly proportional to the product of their masses and is inversely proportional to the
square of the distance between them.
F?m
1
m
2
and F?
1
r
2
so F?
m
1
m
2
r
2
?F=-
Gm
1
m
2
r
2
r ˆ[G= Universal gravitational constant ]
{Note: This formula is only applicable for spherical symmetric masses or point masses.}
VECTOR FORM OF NEWTON'S LAW OF GRAVITATION:
Let ???
12
= Displacement vector from ?? 1
to ?? 2
r ?
21
= Displacement vector from m
2
to m
1
F
??
21
= Gravitational force exerted on m
2
by m
1
F
??
12
= Gravitational force exerted on m
1
by m
2
F
??
12
=-
?? m
1
m
2
r
21
2
r ˆ
21
=-
?? m
1
m
2
r
21
3
r ?
21
Negative sign shows that:
(i) The direction of ???
12
is opposite to that ??ˆ
21
(ii) The gravitational force is attractive in nature
Similarly F
??
21
=-
Gm
1
m
2
r
12
2
r ˆ
12
or F
??
21
=-
Gm
1
m
2
r
12
3
r ?
12
?F
??
12
=-F
??
21
The gravitational force between two bodies are equal in magnitude and opposite in
direction.
GRAVITATIONAL CONSTANT "G"
? Gravitational constant is a scalar quantity.
? Unit: S I: G=6.67×10
-11
N-m
2
/kg
2
CGS: 6.67×10
-8
dyne- -cm
2
/g
2
Dimensions: M
-1
L
3
T
-2
? Its value is the same throughout the universe, G does not depend on the nature
and size of the bodies, it also does not depend upon the nature of the medium
between the bodies.
? Its value was first found out by the scientist "Henry Cavendish" with the help of
the "Torsion Balance" experiment.
? Value of G is small therefore gravitational force is weaker than electrostatic and
nuclear forces.
Example. Two particles of masses 1 kg and 2 kg are placed at a separation of 50 cm .
Assuming that the only forces acting on the particles are their mutual gravitation, find
the initial acceleration of heavier particle.
Solution: Force exerted by one particle on another ?? =
Gm
1
m
2
r
2
=
6.67×10
-11
×1×2
(0.5)
2
=5.3×
10
-10
N
Acceleration of heavier particle =
?? m
2
=
5.3×10
-10
2
=2.65×10
-10
ms
-2
This example shows that gravitation is very weak but only this force keep bind our solar
system and also this universe, all galaxies, and another interstellar system.
Page 3
GRAVITATION
THE DISCOVERY OF THE LAW OF GRAVITATION
The way the law of universal gravitation was discovered is often considered the paradigm
of modern scientific technique. The major steps involved were
? The hypothesis about planetary motion given by Nicolaus Copernicus (1473-
1543).
? The careful experimental measurements of the positions of the planets and the
Sun by Tycho Brahe (1546-1601).
? Analysis of the data and the formulation of empirical laws by Johannes Kepler
(1571-1630).
? The development of a general theory by Isaac Newton (1642-1727).
NEWTON'S LAW OF GRAVITATION
It states that everybody in the universe attracts every other body with a force that is
directly proportional to the product of their masses and is inversely proportional to the
square of the distance between them.
F?m
1
m
2
and F?
1
r
2
so F?
m
1
m
2
r
2
?F=-
Gm
1
m
2
r
2
r ˆ[G= Universal gravitational constant ]
{Note: This formula is only applicable for spherical symmetric masses or point masses.}
VECTOR FORM OF NEWTON'S LAW OF GRAVITATION:
Let ???
12
= Displacement vector from ?? 1
to ?? 2
r ?
21
= Displacement vector from m
2
to m
1
F
??
21
= Gravitational force exerted on m
2
by m
1
F
??
12
= Gravitational force exerted on m
1
by m
2
F
??
12
=-
?? m
1
m
2
r
21
2
r ˆ
21
=-
?? m
1
m
2
r
21
3
r ?
21
Negative sign shows that:
(i) The direction of ???
12
is opposite to that ??ˆ
21
(ii) The gravitational force is attractive in nature
Similarly F
??
21
=-
Gm
1
m
2
r
12
2
r ˆ
12
or F
??
21
=-
Gm
1
m
2
r
12
3
r ?
12
?F
??
12
=-F
??
21
The gravitational force between two bodies are equal in magnitude and opposite in
direction.
GRAVITATIONAL CONSTANT "G"
? Gravitational constant is a scalar quantity.
? Unit: S I: G=6.67×10
-11
N-m
2
/kg
2
CGS: 6.67×10
-8
dyne- -cm
2
/g
2
Dimensions: M
-1
L
3
T
-2
? Its value is the same throughout the universe, G does not depend on the nature
and size of the bodies, it also does not depend upon the nature of the medium
between the bodies.
? Its value was first found out by the scientist "Henry Cavendish" with the help of
the "Torsion Balance" experiment.
? Value of G is small therefore gravitational force is weaker than electrostatic and
nuclear forces.
Example. Two particles of masses 1 kg and 2 kg are placed at a separation of 50 cm .
Assuming that the only forces acting on the particles are their mutual gravitation, find
the initial acceleration of heavier particle.
Solution: Force exerted by one particle on another ?? =
Gm
1
m
2
r
2
=
6.67×10
-11
×1×2
(0.5)
2
=5.3×
10
-10
N
Acceleration of heavier particle =
?? m
2
=
5.3×10
-10
2
=2.65×10
-10
ms
-2
This example shows that gravitation is very weak but only this force keep bind our solar
system and also this universe, all galaxies, and another interstellar system.
Example. Two stationary particles of masses ?? 1
and ?? 2
are at a distance 'd' apart. A
third particle lying on the line joining the particles, experiences no resultant
gravitational forces. What is the distance of this particle from?
Solution: The force on ?? towards ?? 1
is ?? 1
=
?? ?? 1
?? ?? 2
The force on ?? towards ?? 2
is ?? 2
=
GM
2
m
( d-r)
2
According to question net force on ?? is zero i.e. ?? 1
=?? 2
?
GM
1
m
r
2
=
GM
2
m
( d-r)
2
?(
d-r
r
)
2
=
M
2
M
1
?
d
r
-1=
vM
2
vM
1
?r=d[
vM
1
vM
1
+vM
2
]
Example. Three particles, each of mass ?? , are situated at the vertices of an equilateral
triangle of side ' ?? '. The only forces acting on the particles are their mutual gravitational
forces. It is desired that each particle moves in a circle while maintaining their original
separation 'a'. Determine the initial velocity that should be given to each particle and
time period of circular motion.
Solution: The resultant force on particle at A due to other two particles is
F
A
=vF
AB
2
+F
AC
2
+2 F
AB
F
AC
cos 60
°
=v3
Gm
2
a
2
… (i) [?F
AB
=F
AC
=
Gm
2
a
2
]
Radius of the circle r=
2
3
×asin 60
°
=
a
v3
If each particle is given a tangential velocity v,
So that F acts as the centripetal force,
Now
?? ?? 2
?? =v3
?? ?? 2
?? (???? )
Page 4
GRAVITATION
THE DISCOVERY OF THE LAW OF GRAVITATION
The way the law of universal gravitation was discovered is often considered the paradigm
of modern scientific technique. The major steps involved were
? The hypothesis about planetary motion given by Nicolaus Copernicus (1473-
1543).
? The careful experimental measurements of the positions of the planets and the
Sun by Tycho Brahe (1546-1601).
? Analysis of the data and the formulation of empirical laws by Johannes Kepler
(1571-1630).
? The development of a general theory by Isaac Newton (1642-1727).
NEWTON'S LAW OF GRAVITATION
It states that everybody in the universe attracts every other body with a force that is
directly proportional to the product of their masses and is inversely proportional to the
square of the distance between them.
F?m
1
m
2
and F?
1
r
2
so F?
m
1
m
2
r
2
?F=-
Gm
1
m
2
r
2
r ˆ[G= Universal gravitational constant ]
{Note: This formula is only applicable for spherical symmetric masses or point masses.}
VECTOR FORM OF NEWTON'S LAW OF GRAVITATION:
Let ???
12
= Displacement vector from ?? 1
to ?? 2
r ?
21
= Displacement vector from m
2
to m
1
F
??
21
= Gravitational force exerted on m
2
by m
1
F
??
12
= Gravitational force exerted on m
1
by m
2
F
??
12
=-
?? m
1
m
2
r
21
2
r ˆ
21
=-
?? m
1
m
2
r
21
3
r ?
21
Negative sign shows that:
(i) The direction of ???
12
is opposite to that ??ˆ
21
(ii) The gravitational force is attractive in nature
Similarly F
??
21
=-
Gm
1
m
2
r
12
2
r ˆ
12
or F
??
21
=-
Gm
1
m
2
r
12
3
r ?
12
?F
??
12
=-F
??
21
The gravitational force between two bodies are equal in magnitude and opposite in
direction.
GRAVITATIONAL CONSTANT "G"
? Gravitational constant is a scalar quantity.
? Unit: S I: G=6.67×10
-11
N-m
2
/kg
2
CGS: 6.67×10
-8
dyne- -cm
2
/g
2
Dimensions: M
-1
L
3
T
-2
? Its value is the same throughout the universe, G does not depend on the nature
and size of the bodies, it also does not depend upon the nature of the medium
between the bodies.
? Its value was first found out by the scientist "Henry Cavendish" with the help of
the "Torsion Balance" experiment.
? Value of G is small therefore gravitational force is weaker than electrostatic and
nuclear forces.
Example. Two particles of masses 1 kg and 2 kg are placed at a separation of 50 cm .
Assuming that the only forces acting on the particles are their mutual gravitation, find
the initial acceleration of heavier particle.
Solution: Force exerted by one particle on another ?? =
Gm
1
m
2
r
2
=
6.67×10
-11
×1×2
(0.5)
2
=5.3×
10
-10
N
Acceleration of heavier particle =
?? m
2
=
5.3×10
-10
2
=2.65×10
-10
ms
-2
This example shows that gravitation is very weak but only this force keep bind our solar
system and also this universe, all galaxies, and another interstellar system.
Example. Two stationary particles of masses ?? 1
and ?? 2
are at a distance 'd' apart. A
third particle lying on the line joining the particles, experiences no resultant
gravitational forces. What is the distance of this particle from?
Solution: The force on ?? towards ?? 1
is ?? 1
=
?? ?? 1
?? ?? 2
The force on ?? towards ?? 2
is ?? 2
=
GM
2
m
( d-r)
2
According to question net force on ?? is zero i.e. ?? 1
=?? 2
?
GM
1
m
r
2
=
GM
2
m
( d-r)
2
?(
d-r
r
)
2
=
M
2
M
1
?
d
r
-1=
vM
2
vM
1
?r=d[
vM
1
vM
1
+vM
2
]
Example. Three particles, each of mass ?? , are situated at the vertices of an equilateral
triangle of side ' ?? '. The only forces acting on the particles are their mutual gravitational
forces. It is desired that each particle moves in a circle while maintaining their original
separation 'a'. Determine the initial velocity that should be given to each particle and
time period of circular motion.
Solution: The resultant force on particle at A due to other two particles is
F
A
=vF
AB
2
+F
AC
2
+2 F
AB
F
AC
cos 60
°
=v3
Gm
2
a
2
… (i) [?F
AB
=F
AC
=
Gm
2
a
2
]
Radius of the circle r=
2
3
×asin 60
°
=
a
v3
If each particle is given a tangential velocity v,
So that F acts as the centripetal force,
Now
?? ?? 2
?? =v3
?? ?? 2
?? (???? )
Time period T=
2?? r
v
=
2?? a
v3
v
a
Gm
=2?? v
a
3
3Gm
? Fractional forces are central forces as they act along the line joining the centers of
two bodies.
? The gravitational forces are conservative forces so work done by gravitational
force does not depends upon path and therefore if any particle moves along a
closed path under the action of gravitational force then the work done by this
force is always zero.
? The total gravitational force on one particle due to a number of particles is the
resultant of forces of attraction exerted on the given particle due to individual
particles i.e. ???
=???
1
+???
2
+???
3
+ means the principle of superposition is valid.
GRAVITATIONAL FIELD
The gravitational field is the space around a mass or an assembly of masses over which it
can exert gravitational forces on other masses.
Theoretically speaking, the gravitational field extends up to infinity. However, in actual
practice, the gravitational field may become too weak to be measured beyond a particular
distance.
Gravitational Field Intensity [g or E
g
]
Gravitational force acting per unit mass at any point in the gravitational field is called
Gravitational field intensity.
?? =
?????? ?? 2
/?? =
????
?? 2
Vector form :??? =
???
?? or ???=-
????
?? 2
??ˆ
Page 5
GRAVITATION
THE DISCOVERY OF THE LAW OF GRAVITATION
The way the law of universal gravitation was discovered is often considered the paradigm
of modern scientific technique. The major steps involved were
? The hypothesis about planetary motion given by Nicolaus Copernicus (1473-
1543).
? The careful experimental measurements of the positions of the planets and the
Sun by Tycho Brahe (1546-1601).
? Analysis of the data and the formulation of empirical laws by Johannes Kepler
(1571-1630).
? The development of a general theory by Isaac Newton (1642-1727).
NEWTON'S LAW OF GRAVITATION
It states that everybody in the universe attracts every other body with a force that is
directly proportional to the product of their masses and is inversely proportional to the
square of the distance between them.
F?m
1
m
2
and F?
1
r
2
so F?
m
1
m
2
r
2
?F=-
Gm
1
m
2
r
2
r ˆ[G= Universal gravitational constant ]
{Note: This formula is only applicable for spherical symmetric masses or point masses.}
VECTOR FORM OF NEWTON'S LAW OF GRAVITATION:
Let ???
12
= Displacement vector from ?? 1
to ?? 2
r ?
21
= Displacement vector from m
2
to m
1
F
??
21
= Gravitational force exerted on m
2
by m
1
F
??
12
= Gravitational force exerted on m
1
by m
2
F
??
12
=-
?? m
1
m
2
r
21
2
r ˆ
21
=-
?? m
1
m
2
r
21
3
r ?
21
Negative sign shows that:
(i) The direction of ???
12
is opposite to that ??ˆ
21
(ii) The gravitational force is attractive in nature
Similarly F
??
21
=-
Gm
1
m
2
r
12
2
r ˆ
12
or F
??
21
=-
Gm
1
m
2
r
12
3
r ?
12
?F
??
12
=-F
??
21
The gravitational force between two bodies are equal in magnitude and opposite in
direction.
GRAVITATIONAL CONSTANT "G"
? Gravitational constant is a scalar quantity.
? Unit: S I: G=6.67×10
-11
N-m
2
/kg
2
CGS: 6.67×10
-8
dyne- -cm
2
/g
2
Dimensions: M
-1
L
3
T
-2
? Its value is the same throughout the universe, G does not depend on the nature
and size of the bodies, it also does not depend upon the nature of the medium
between the bodies.
? Its value was first found out by the scientist "Henry Cavendish" with the help of
the "Torsion Balance" experiment.
? Value of G is small therefore gravitational force is weaker than electrostatic and
nuclear forces.
Example. Two particles of masses 1 kg and 2 kg are placed at a separation of 50 cm .
Assuming that the only forces acting on the particles are their mutual gravitation, find
the initial acceleration of heavier particle.
Solution: Force exerted by one particle on another ?? =
Gm
1
m
2
r
2
=
6.67×10
-11
×1×2
(0.5)
2
=5.3×
10
-10
N
Acceleration of heavier particle =
?? m
2
=
5.3×10
-10
2
=2.65×10
-10
ms
-2
This example shows that gravitation is very weak but only this force keep bind our solar
system and also this universe, all galaxies, and another interstellar system.
Example. Two stationary particles of masses ?? 1
and ?? 2
are at a distance 'd' apart. A
third particle lying on the line joining the particles, experiences no resultant
gravitational forces. What is the distance of this particle from?
Solution: The force on ?? towards ?? 1
is ?? 1
=
?? ?? 1
?? ?? 2
The force on ?? towards ?? 2
is ?? 2
=
GM
2
m
( d-r)
2
According to question net force on ?? is zero i.e. ?? 1
=?? 2
?
GM
1
m
r
2
=
GM
2
m
( d-r)
2
?(
d-r
r
)
2
=
M
2
M
1
?
d
r
-1=
vM
2
vM
1
?r=d[
vM
1
vM
1
+vM
2
]
Example. Three particles, each of mass ?? , are situated at the vertices of an equilateral
triangle of side ' ?? '. The only forces acting on the particles are their mutual gravitational
forces. It is desired that each particle moves in a circle while maintaining their original
separation 'a'. Determine the initial velocity that should be given to each particle and
time period of circular motion.
Solution: The resultant force on particle at A due to other two particles is
F
A
=vF
AB
2
+F
AC
2
+2 F
AB
F
AC
cos 60
°
=v3
Gm
2
a
2
… (i) [?F
AB
=F
AC
=
Gm
2
a
2
]
Radius of the circle r=
2
3
×asin 60
°
=
a
v3
If each particle is given a tangential velocity v,
So that F acts as the centripetal force,
Now
?? ?? 2
?? =v3
?? ?? 2
?? (???? )
Time period T=
2?? r
v
=
2?? a
v3
v
a
Gm
=2?? v
a
3
3Gm
? Fractional forces are central forces as they act along the line joining the centers of
two bodies.
? The gravitational forces are conservative forces so work done by gravitational
force does not depends upon path and therefore if any particle moves along a
closed path under the action of gravitational force then the work done by this
force is always zero.
? The total gravitational force on one particle due to a number of particles is the
resultant of forces of attraction exerted on the given particle due to individual
particles i.e. ???
=???
1
+???
2
+???
3
+ means the principle of superposition is valid.
GRAVITATIONAL FIELD
The gravitational field is the space around a mass or an assembly of masses over which it
can exert gravitational forces on other masses.
Theoretically speaking, the gravitational field extends up to infinity. However, in actual
practice, the gravitational field may become too weak to be measured beyond a particular
distance.
Gravitational Field Intensity [g or E
g
]
Gravitational force acting per unit mass at any point in the gravitational field is called
Gravitational field intensity.
?? =
?????? ?? 2
/?? =
????
?? 2
Vector form :??? =
???
?? or ???=-
????
?? 2
??ˆ
Gravitational field intensity is a vector quantity having dimension [LT
-2
] and unit N/kg .
? Since the force between two point masses is having the similar expression as that
of force between two point charges, we can write the gravitational field &
gravitational potential in the same manner as the electric field & electric
potential.
Gravitational Potential:
Gravitational field around a material body can be described not only by gravitational
intensity ?? , but also by a scalar function, the gravitational potential V. Gravitational
potential is the amount of work done in bringing a body of unit mass from infinity to that
point without changing its kinetic energy.
V=
W
m
This work done is the measure of gravitational potential at point (P)
?V
P
=-
GM
r
(I)
(1) Dini Charge
(a) E=
kQ
r
2
r
(2) Uniform charged ring
(a) =
kQx
(i
2
+x
2
)
3/2
on axis ?? when ?? =
?? v2
(b) ?? =
kQ
vy
2
+x
2
on axis,
kQ
r
at center
(3) Uniform linear charge
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