Newton and Gravity

1. Newton and Gravity

2. Isaac Newton (1642-1727) • Galileo found that bodies with different masses experienced the same acceleration when dropped to the ground. But he didn’t know why. • Kepler discovered that the motions of the planets were perfectly reproduced by 3 mathematical relations. Like Galileo, Kepler didn’t know why these relations worked. • Isaac Newton was able to explain the results of Galileo and Kepler, and many other phenomena in nature, with a few general principles

3. Newton’s Concepts • m(mass): How much stuff something contains • v (velocity): A body’s speed and direction 3)a(acceleration): The change in a body’s velocity 4) F (force): What is needed to change a body’s velocity

4. A body’s velocity will remain constant, unless acted upon by an outside force = inertia Newton’s Laws of Motion

5. A body’s velocity will remain constant, unless acted upon by an outside force = inertia Newton’s Laws of Motion • A body’s acceleration depends on the force acting upon it, and will be in the direction of that force. Its resistance to acceleration depends on its mass. In equation form, this is F = m a • For every force, there is an equal and opposite force.

6. Newton’s Law of Gravity There is an attractive force between two bodies called gravity. The force of gravity depends on the masses of the two bodies, and their separation (squared); the larger the mass, the greater the attraction; the larger the separation, the smaller the attraction. G m1 m2 Note that the word “separation” means the distance between the centers of the two bodies. F =  d2

7. Galileo found that objects with different masses feel same acceleration from the Earth. Why is that? m M = Earth’s mass Newton’s 2nd law: F = m a Newton’s law of gravity: F = G m M / d2 F = m a = G m M/ d2 a = G M / d2 An object’s acceleration does not depend on its own mass. It depends on the mass of the other object (the Earth, in this case).

8. Example of Gravity – a Thrown Ball When you throw a ball, there are 2 motions: horizontal & vertical. The horizontal motion obeys Newton’s first law (bodies in motion will stay in motion). The attractive force of gravity causes the upward motion to decelerate, and then change direction. You see the composite of the two behaviors.

9. Example of Gravity – a Thrown Ball

10. Example of Gravity – Weightlessness You feel weight because of Newton’s third law. Gravity is pulling you down, but the ground is not allowing you to fall. It must therefore be exerting a force on you to keep you from falling. That force is the weight that you feel. If you were allowed to fall, you would not feel any weight. So when you are in free-fall, you feel weightlessness.

11. Example of Gravity – Weightlessness As an example, a sky diver is in free fall towards the earth, and therefore feels weightlessness. gravity

12. Example of Gravity – Weightlessness If an additional force is applied to the sky diver that is not in the direction of gravity, he will fall on a curved path because of inertia (Newton’s 1st law). inertia gravity

13. Example of Gravity – Orbits If the size of the force is just right, the sky diver falls on a curved path that never reaches the ground and loops back on itself. This is an orbit. The sky diver (or astronaut) experiences weightlessness indefinitely. inertia gravity

14. Example of Gravity – Orbits If the Earth had been born at rest relative to the Sun, it would have fallen immediately into the Sun.

15. Example of Gravity – Binary Stars Because planets are much less massive than the Sun, they induce very little acceleration in the Sun, so the Sun barely moves and has a very small “orbit”, while the planets are move a lot and have large orbits because of the strong acceleration induced by the Sun.

16. Example of Gravity – Binary Stars If the Sun was orbited by larger bodies, like other stars, it would move much more in its orbit. http://astro.unl.edu/naap/esp/animations/radialVelocitySimulator.html