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Understanding Newton's Law of Universal Gravitation: Inverse Square Law & Applications - P, Study notes of Physics

An in-depth exploration of newton's law of universal gravitation, an inverse square law that describes the force of attraction between every particle in the universe. Topics covered include the mathematical expression of the law, the concept of gravitational constant, the forces exerted between particles, and the comparison of g and g. Additionally, the document discusses the verification of the law through newton's experiments and kepler's laws.

Typology: Study notes

Pre 2010

Uploaded on 08/09/2009

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Newton’s Law of Universal
Gravitation (Ch 13)
Every particle in the Universe attracts every other
particle with a force that is directly proportional to the
product of their masses and inversely proportional to
the distance between them
G is the universal gravitational constant
G = 6.673 x 10-11 Nm2 / kg2
Law of Gravitation, cont
This is an example of an inverse square law
The magnitude of the force varies as the inverse
square of the separation of the particles
The law can also be expressed in vector form
Notation
F12 is the force exerted by particle 1 on
particle 2
The negative sign in the vector form of the
equation indicates that particle 2 is attracted
toward particle 1
F21 is the force exerted by particle 2 on
particle 1
More About Forces
F12 = -F21
The forces form a Newton’s
Third Law action-reaction pair
Gravitation is a field force that
always exists between two
particles, regardless of the
medium between them
The force decreases rapidly
as distance increases
A consequence of the inverse
square law
pf3
pf4
pf5

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Newton’s Law of Universal

Gravitation (Ch 13)

  • Every particle in the Universe attracts every other particle with a force that is directly proportional to the product of their masses and inversely proportional to the distance between them
  • G is the universal gravitational constant G = 6.673 x 10-11^ N⋅m^2 / kg^2

Law of Gravitation, cont

• This is an example of an inverse square law

  • The magnitude of the force varies as the inverse square of the separation of the particles

• The law can also be expressed in vector form

Notation

• F 12 is the force exerted by particle 1 on

particle 2

• The negative sign in the vector form of the

equation indicates that particle 2 is attracted

toward particle 1

• F 21 is the force exerted by particle 2 on

particle 1

More About Forces

• F 12 = - F 21

  • The forces form a Newton’s Third Law action-reaction pair
  • Gravitation is a field force that always exists between two particles, regardless of the medium between them
  • The force decreases rapidly as distance increases
  • A consequence of the inverse square law

G vs. g

• Always distinguish between G and g

• G is the universal gravitational constant

  • It is the same everywhere

• g is the acceleration due to gravity

  • g = 9.80 m/s^2 at the surface of the Earth
  • g will vary by location

Gravitational Force Due to a

Distribution of Mass

• The gravitational force exerted by a finite-

size, spherically symmetric mass distribution

on a particle outside the distribution is the

same as if the entire mass of the distribution

were concentrated at the center

• For the Earth,

Newton’s Verification

  • Developed theory at age 23!
  • He compared the acceleration of the Moon in its orbit with the acceleration of an object falling near the Earth’s surface
  • He calculated the centripetal acceleration of the Moon from its distance and period
  • The high degree of agreement between the two techniques provided evidence of the inverse square nature of the law (^) Newton’s Canon

Moon’s Acceleration

• Newton looked at proportionality of

accelerations between the Moon and objects

on the Earth

g Above the Earth’s Surface

• If an object is some distance h above the

Earth’s surface, r becomes RE + h

• This shows that g decreases with increasing

altitude

• As r → ∞, the weight of the object approaches

zero

Variation of g with Height

Ch 13: Question 4

• The gravitational force that the Sun exerts on

the Moon is about twice as great as the

gravitational force that the Earth exerts on the

Moon. Why doesn’t the Sun pull the Moon

away from the Earth during a total eclipse of

the Sun?

Kepler’s Laws, Introduction

• Johannes Kepler was a German astronomer

• He was Tycho Brahe’s assistant

  • Brahe was the last of the “naked eye” astronomers

• Kepler analyzed Brahe’s data and formulated

three laws of planetary motion

Kepler’s Laws

• Kepler’s First Law

  • All planets move in elliptical orbits with the Sun at one focus

• Kepler’s Second Law

  • The radius vector drawn from the Sun to a planet sweeps out equal areas in equal time intervals

• Kepler’s Third Law

  • The square of the orbital period of any planet is proportional to the cube of the semimajor axis of the elliptical orbit

Notes About Ellipses

  • F 1 and F 2 are each a focus of the ellipse - They are located a distance c from the center
  • The longest distance through the center is the major axis - a is the semimajor axis
  • The shortest distance through the center is the minor axis - b is the semiminor axis
  • eccentricity , e = c / a
    • For a circle, e = 0
    • For ellipses, 0 < e < 1

Planetary Orbits

• The Sun is at one focus

  • Nothing is located at the other focus

• Aphelion is the point farthest away from the Sun

  • The distance for aphelion is a + c
    • For an orbit around the Earth, this point is called the apogee

• Perihelion is the point nearest the Sun

  • The distance for perihelion is ac
    • For an orbit around the Earth, this point is called the perigee

Kepler’s First Law

  • A circular orbit is a special case of the general elliptical orbits
  • Is a direct result of the inverse square nature of the gravitational force
  • Elliptical (and circular) orbits are allowed for bound objects - A bound object repeatedly orbits the center - An unbound object would pass by and not return - These objects could have paths that are parabolas ( e = 1) and hyperbolas ( e > 1)

Example, Mass of the Sun

• Using the distance between the Earth and the

Sun, and the period of the Earth’s orbit,

Kepler’s Third Law can be used to find the

mass of the Sun

• Similarly, the mass of any object being

orbited can be found if you know information

about objects orbiting it

Example, Geosynchronous

Satellite

  • A geosynchronous satellite appears to remain over the same point on the Earth
  • The gravitational force supplies a centripetal force
  • You can find h or v