Chapter 2GravityThe Problem of Astronomical MotionInertiaInertia and Newton’s First LawNewton’s First LawAstronomical MotionGravity is that force!Orbital Motion and GravityOrbital Motion Using Newton’s First LawSlide 11Newton’s Second Law: MotionNewton’s 2nd Law: AccelerationNewton’s Second Law: MassNewton’s Second Law of MotionF = maNewton’s Law of Universal GravityNewton’s Third Law of MotionMeasuring an Object’s Mass Using Orbital MotionSlide 20Surface GravitySurface Gravity CalculationsEscape VelocitySlide 24Escape Velocity CalculationSlide 26Chapter 2Gravity and MotionCopyright (c) The McGraw-Hill Companies, Inc. Permission required for reproduction or display.Gravity•Gravity gives the Universe its structure–It is a universal force that causes all objects to pull on all other objects everywhere–It holds objects together–It is responsible for holding the Earth in its orbit around the Sun, the Sun in its orbit around the Milky Way, and the Milky Way in its path within the Local GroupThe Problem of Astronomical Motion•Astronomers of antiquity did not connect gravity and astronomical motion•Galileo investigated this connection with experiments using projectiles and balls rolling down planks•He put science on a course to determine laws of motion and to develop the scientific methodInertia•Galileo established the idea of inertia–A body at rest tends to remain at rest–A body in motion tends to remain in motion–Through experiments with inclined planes, Galileo demonstrated the idea of inertia and the importance of forces (friction)Inertia and Newton’s First Law•This concept was incorporated in Newton’s First Law of Motion:A body continues in a state of rest or uniform motion in a straight line unless made to change that state by forces acting on itNewton’s First Law•Important ideas of Newton’s First Law–Force: A push or a pull–The force referred to is a net force–The law implies that if an object is not moving with constant velocity, then a nonzero net force must be presentAstronomical Motion•As seen in Chapter 1, planets move along curved (elliptical) paths, or orbits.•Speed and direction is changing•Must there be a force at work?•Yes!Eqn. of ellipseGravity is that force!Orbital Motion and Gravity•Although not the first to propose gravity as being responsible for celestial motion, Newton was the first to:–Spell out the properties of gravity–Write the equations of gravity-induced motion•Newton deduced that:–The Moon’s motion could be explained by the existence of a force (to deviate the Moon from a straight inertial trajectory) and that such a force decreased with distance–Orbital motion could be understood as a projectile moving “parallel” to the Earth’s surface at such a speed that its gravitational deflection toward the surface is offset by the surface’s curvature away from the projectileOrbital Motion Using Newton’s First Law•A cannonball fired at slow speed experiences one force – gravity, pulling it downward•A cannonball fired at a higher speed feels the same force, but goes fartherOrbital Motion Using Newton’s First Law•At a sufficiently high speed, the cannonball travels so far that the ground curves out from under it.•The cannonball literally misses the ground!•The ball, now in orbit, still experiences the pull of gravity!Newton’s Second Law: Motion•Motion–An object is said to be in uniform motion if its speed and direction remain unchanged–An object in uniform motion is said to have a constant velocity–A force will cause an object to have non-uniform motion, a changing velocity–Acceleration is defined as a change in velocityNewton’s 2nd Law: Acceleration•Acceleration–An object increasing or decreasing in speed along a straight line is accelerating–An object with constant speed moving is a circle is accelerating–Acceleration is produced by a force and experiments show the two are proportionalNewton’s Second Law: Mass•Mass–Mass is the amount of matter an object contains–Technically, mass is a measure of an object’s inertia–Mass is generally measured in kilograms–Mass should not be confused with weight, which is a force related to gravity – weight may change from place to place, but mass does notNewton’s Second Law of Motion•Equivalently, the amount of acceleration (a) that an object undergoes is proportional to the force applied (F) and inversely proportional to the mass (m) of the object–This equation applies for any force, gravitational or otherwiseF = maF = maF = maNewton’s Law of Universal Gravity•Everything attracts everything else!!Newton’s Third Law of Motion•When two objects interact, they create equal and opposite forces on each other•This is true for any two objects, including the Sun and the Earth!Measuring an Object’s Mass Using Orbital Motion•Basic Setup of an Orbital Motion Problem–Assume a small mass object orbits around a much more massive object–Massive object can be assumed at rest (very little acceleration)–Assume orbit shape of small mass is a circle centered on large mass•Using Newton’s Second Law–Acceleration in a circular orbit must be:a = v2/r where v is the constant orbital speed and r is the radius of the orbit–The force is that of gravityMeasuring an Object’s Mass Using Orbital Motion•Method of Solution–Equate F = mv2/r to F = GMm/r2 and solve for v:v = (GM/r)1/2–One can also solve for M:M = (v2r)/G–v can be expressed in terms of the orbital period (P) on the small mass and its orbital radius:v = 2r/P–Combining these last two equations:M = (42r3)/(GP2)–This last equation in known as Kepler’s modified third law and is often used to calculate the mass of a large celestial object from the orbital period and radius of a much smaller massSurface Gravity•Surface gravity is the acceleration a mass undergoes at the surface of a celestial object (e.g., an asteroid, planet, or star)•Surface gravity:–Determines the weight of a mass at a celestial object’s surface–Influences the shape of celestial objects–Influences whether or not a celestial object has an atmosphereSurface Gravity Calculations•Surface gravity is determined from Newton’s Second Law and the Law of Gravity:ma = GMm/R2where M and R are the mass and radius of the celestial object, and m is the mass of the object whose acceleration a we wish to know•The surface gravity, denoted by