Understanding Planetary Orbits & Object Motion: Kepler's & Newton's Laws, Lecture notes of Physics

An overview of kepler's laws of planetary motion and their significance in the development of newton's laws of motion. Kepler's laws describe the elliptical orbits of planets around the sun and their relationship to their distances and orbital periods. Newton's laws, in turn, explain the relationship between an object's motion and the forces acting upon it. The document also covers the concepts of speed, velocity, acceleration, free falling bodies, and projectile motion.

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Kepler’s Planetary Motion
Kepler’s laws of planetary motion, in astronomy and
classical physics, laws describing the motions of the planets in
the solar system. They were derived by the German
astronomer Johannes Kepler, whose analysis of the observations of
the 16th-century Danish astronomer Tycho Brahe enabled him to
announce his first two laws in the year 1609 and a third law
nearly a decade later, in 1618. Kepler himself never numbered
these laws or specially distinguished them from his other
discoveries
Kepler’s three laws of planetary motion can be stated as follows:
1) All planets move about the Sun in elliptical orbits, having
the Sun as one of the foci.
2) A radius vector joining any planet to the Sun sweeps out equal
areas in equal lengths of time.
3) The squares of the sidereal periods (of revolution) of the
planets are directly proportional to the cubes of their mean
distances from the Sun.
Knowledge of these laws, especially the second (the law of
areas), proved crucial to Sir Isaac Newton in 1684–85, when he
formulated his famous law of gravitation between Earth and the
Moon and between the Sun and the planets, postulated by him to
have validity for all objects anywhere in the universe. Newton
showed that the motion of bodies subject to central
gravitational force need not always follow the elliptical orbits
specified by the first law of Kepler but can take paths defined
by other, open conic curves; the motion can be in parabolic or
hyperbolic orbits, depending on the total energy of the body.
Thus, an object of sufficient energy—e.g., a comet—can enter the
solar system and leave again without returning. From Kepler’s
second law, it may be observed further that the angular
momentum of any planet about an axis through the Sun and
perpendicular to the orbital plane is also unchanging
Most planetary orbits are nearly circular, and careful
observation and calculation are required in order to establish
that they are not perfectly circular. Calculations of the orbit
of Mars, whose published values are somewhat suspect, indicated
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Kepler’s Planetary Motion

Kepler’s laws of planetary motion, in astronomy and classical physics, laws describing the motions of the planets in the solar system. They were derived by the German astronomer Johannes Kepler, whose analysis of the observations of the 16th-century Danish astronomer Tycho Brahe enabled him to announce his first two laws in the year 1609 and a third law nearly a decade later, in 1618. Kepler himself never numbered these laws or specially distinguished them from his other discoveries

Kepler’s three laws of planetary motion can be stated as follows:

  1. All planets move about the Sun in elliptical orbits, having the Sun as one of the foci.

  2. A radius vector joining any planet to the Sun sweeps out equal areas in equal lengths of time.

  3. The squares of the sidereal periods (of revolution) of the planets are directly proportional to the cubes of their mean distances from the Sun.

Knowledge of these laws, especially the second (the law of areas), proved crucial to Sir Isaac Newton in 1684–85, when he formulated his famous law of gravitation between Earth and the Moon and between the Sun and the planets, postulated by him to have validity for all objects anywhere in the universe. Newton showed that the motion of bodies subject to central gravitational force need not always follow the elliptical orbits specified by the first law of Kepler but can take paths defined by other, open conic curves; the motion can be in parabolic or hyperbolic orbits, depending on the total energy of the body. Thus, an object of sufficient energy—e.g., a comet—can enter the solar system and leave again without returning. From Kepler’s second law, it may be observed further that the angular momentum of any planet about an axis through the Sun and perpendicular to the orbital plane is also unchanging

Most planetary orbits are nearly circular, and careful observation and calculation are required in order to establish that they are not perfectly circular. Calculations of the orbit of Mars, whose published values are somewhat suspect, indicated

an elliptical orbit. From this, Johannes Kepler inferred that other bodies in the Solar System, including those farther away from the Sun, also have elliptical orbits.

Newton’s Laws of Motion

The motion of an aircraft through the air can be explained and described by physical principals discovered over 300 years ago by Sir Isaac Newton. Newton worked in many areas of mathematics and physics. He developed the theories of gravitation in 1666, when he was only 23 years old. Some twenty years later, in 1686, he presented his three laws of motion in the "Principia Mathematica Philosophiae Naturalis." Newton's laws of motion are three physical laws that, together, laid the foundation for classical mechanics. They describe the relationship between a body and the forces acting upon it, and its motion in response to those forces.

Newton's first law states that every object will remain at rest or in uniform motion in a straight line unless compelled to change its state by the action of an external force. This is normally taken as the definition of inertia. The key point here is that if there is no net force acting on an object (if all the external forces cancel each other out) then the object will maintain a constant velocity. If that velocity is zero, then the object remains at rest. If an external force is applied, the velocity will change because of the force.

The second law explains how the velocity of an object changes when it is subjected to an external force. The law defines a force to be equal to change in momentum (mass times velocity) per change in time. Newton also developed the calculus of mathematics, and the "changes" expressed in the second law are most accurately defined in differential forms. (Calculus can also be used to determine the velocity and location variations experienced by an object subjected to an external force.) For an object with a constant mass m, the second law states that the force F is the product of an object's mass and its acceleration a: F = m * a

What is Acceleration?

In physics, acceleration is the rate of change of velocity of an object with respect to time. An object's acceleration is the net result of any and all forces acting on the object, as described by Newton's Second Law. The SI unit for acceleration is meter per second squared.

What does Free Falling Bodies mean?

Newtonian physics, free fall is any motion of a body where gravity is the only force acting upon it. In the context of general relativity, where gravitation is reduced to a space-time curvature, a body in free fall has no force acting on it. A free falling object is an object that is falling under the sole influence of gravity. Any object that is being acted upon only by the force of gravity is said to be in a state of free fall. ...Free-falling objects do not encounter air resistance.

What do you mean by Projectile Motion?

Projectile motion is a form of motion experienced by an object or particle that is thrown near the Earth's surface and moves along a curved path under the action of gravity only. This curved path was shown by Galileo to be a parabola. For example, you throw the ball straight upward, or you kick a ball and give it a speed at an angle to the horizontal or you just drop things and make them free fall; all these are examples of projectile motion. In projectile motion, gravity is the only force acting on the object. A projectile is any object that once projected or dropped continues in motion by its own inertia and is influenced only by the downward force of gravity. By definition, a projectile has a single force that acts upon it - the force of gravity. Many projectile^ not^ only^ undergo^ a^ vertical^ motion,^ but also undergo a horizontal motion. That is, as they move upward or downward they are also moving horizontally. They are the two components of the projectile’s motion, horizontal and vertical motion.

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