Lecture 5 Newton -Tides ASTR 340 Fall 2006 Dennis Papadopoulos.
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Transcript of Lecture 5 Newton -Tides ASTR 340 Fall 2006 Dennis Papadopoulos.
Motion at constant acceleration a in meters/sec2
Start with zero velocity. Velocity after time t is v(t)=at.The average speed during this time was vav=(0+at)/2=at/2
The distance traveled s=vavt=at2/2Suppose you accelerate from 0 to 50 m/sec in 10 secsThe distance s will be given byS=(1/2)(5 m/sec2)102= 250 m
The general formula if you start with initial velocity v(0) is
s=v(0)t+(1/2)at2
ACCELERATING MOTION
• N1 with v0 comes directly from Aristotle’s concept (object at rest remains at rest) by applying Galilean Relativity: change to frame with initial v=0 ; F=0 so object remains at rest; change frames back and v= initial v
• N3 is exactly what’s needed to make sure that the total momentum is conserved.
• So… Newton’s laws are related to the symmetry of space and the way that different frames of reference relate to each other.
Conservation Principles
Action=Reaction
If friction and pull balance exactly cart moves with constant velocity otherwise it slows down or accelerates
depending on what dominates
Force and acceleration
Forces between two bodies are equal in magnitude, but the observed reaction --the acceleration -- depends on mass
If a bowling ball and ping-pong ball are pushed apart by spring, the bowling ball will move very little, and the ping-pong ball will move a lot
Forces in a collision are equal in magnitude, too
Velocity, as used in Newton’s laws, includes both a speed and a direction. V and also F and a are vectors.
Any change in direction, even if the speed is constant, requires a force
In particular, motion at constant speed in a circle must involve a force at all times, since the direction is always changing
Circular or Elliptical Motion
NEWTON’S LAW OF UNIVERSAL GRAVITATION
Newton’s law of Gravitation: A particle with mass m1 will attract another particle with mass m2 and distance r with a force F given by
Notes:1. “G” is called the Gravitational constant
(G=6.6710-11 N m2 kg-2)2. This is a universal attraction. Every
particle in the universe attracts every other particle! Often dominates in astronomical settings.
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r
mGmF
Gravitational Mass vs. Weight
3. Defines “gravitational mass”4. Using calculus, it can be shown that a
spherical object with mass M (e.g. Sun, Earth) gravitates like a particle of mass M at the sphere’s center.
2r
GMmF
Apple falls 5 m in one sec
Moon falls about 1.4 mm in one sec away from straight line
Moon
Earth
REM/RE=60
First grand unification
KEPLER’S LAWS EXPLAINED
Kepler’s laws of planetary motion Can be derived from Newton’s laws Just need to assume that planets are attracted to the
Sun by gravity (Newton’s breakthrough). Full proof requires calculus (or very involved geometry)
Planets natural state is to move in a straight line at constant velocity
But, gravitational attraction by Sun is always making it swerve off course
Newton’s law (1/r2) is exactly what’s needed to make this path be a perfect ellipse – hence Kepler’s 1st law.(use calculus)
The fact that force is always directed towards Sun gives Kepler’s 2nd law (conservation of angular momentum)
Newton’s law gives formula for period of orbit
32
2
)(
4R
MMGP
planetsun
TIDES
Daily tide twice Why? 1/R2 law
Moon
Earth
Water pulled stronger thanthe earth
Earth pulled stronger thanthe water
TIDES
Twice monthly Spring Tides (unrelated to Spring) andTwice monthly Neap Tides
Sun
moon
Earth
moon
Full moon – extra low tides
Earth New moon Extra high tides