6.5 Newton's Law of Gravity Notes

Newton's Law of Gravity

  • Isaac Newton developed the concept of gravity as a universal force affecting all objects in the universe.

  • The same force that causes an apple to fall also keeps the moon in orbit.

Universal Law of Gravitation

  • Every object attracts every other object with a force that varies based on:

    • The mass of the objects (directly proportional to the product of their masses).

    • The distance between them (inversely proportional to the square of the distance).

    • Mathematically, F=Gm<em>1m</em>2r2F = G \frac{m<em>1 m</em>2}{r^2} where:

    • FF is the gravitational force,

    • GG is the gravitational constant (G=6.67×1011 N m2/kg2G = 6.67 \times 10^{-11} \text{ N m}^2 / \text{kg}^2),

    • m<em>1m<em>1 and m</em>2m</em>2 are the masses, and

    • rr is the distance between the centers of the masses.

Inverse Square Law

  • As distance rr increases, gravitational force decreases dramatically:

    • Doubling the distance reduces the force by a factor of four (i.e., gravity behaves according to an inverse square relationship).

Inverse Relationship Concept

  • If yy is inversely proportional to x2x^2, we can express this as:

    • y=ax2y = \frac{a}{x^2}

    • If xx increases by a factor of cc, yy decreases by a factor of c2c^2.

Gravitational Force Examples

  • The gravitational force between ordinary objects is typically small unless one or both masses are large (e.g., Earth).

  • Weight on other celestial bodies varies due to different gravitational accelerations (e.g., on the moon or other planets).

    • g<em>moon=1.62 m/s2g<em>{moon} = 1.62 \text{ m/s}^2 and g</em>Earth=9.8 m/s2g</em>{Earth} = 9.8 \text{ m/s}^2.

Calculating Gravitational Force

  • The gravitational force can be calculated for a person on Earth using:

    • F=GM<em>Earthm</em>personREarth2F = G \frac{M<em>{Earth} m</em>{person}}{R_{Earth}^2}, where the mass of Earth and radius are involved.

Variation in Gravity

  • Earth's gravity varies slightly due to its uneven density, but this variation is generally negligible for basic calculations.

Orbiting Objects

  • Objects in orbit are not weightless but are in free fall.

  • The period of orbit and gravitational force can be correlated using gravitational biomechanics.