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Newton's Law of Universal Gravitation

During the plague years 1665-1666, Newton came to understand the mechanism that tied the universe together according to a rule. It would appear that he approached the problem from opposite venues. He had been studying the path of the moon. What is now known as Newton's first law suggests that if an object is moving with uniform speed in a straight line, then Fnet must be zero. That implies that if the path of an object is not a straight line, then Fnet is not zero. From that conclusion, we infer from the second law that, because Fnet is not zero, the object must be accelerating -- even if it is moving at a constant speed! Further, the acceleration must point in the same direction as Fnet. From this Newton concluded that there must be something at the center of the moon's path that supplied Fnet; but the only thing there was the Earth.

Now comes the apocryphal story of Newton sitting in his garden when an apple falls from tree. He ruminated on how far up the tree and into the sky did this force go. He speculated that the force might even extend to the moon and set about calculating the acceleration that the moon should experience, and compared that number to his estimate of what the Earth's acceleration due to gravity would be at that distance and "...found that they answered pretty nearly."  Newton did the proof geometrically using wretched British units. We can do it algebraically with metric units and arrive at a conclusion similar to Newton's.

 Part 1. At the surface of the Earth (one Earth radius from the center of the planet), the acceleration due to gravity is g = 9.8 m/s2. At the site of the moon, some 240,000 miles (60 Earth radii ) away, Newton speculated that g = (1/60)2 times 9.8 m/s2. We calculate this quantity g = .00272 m/s^2 Part 2. Now if the moon takes a circular path, it must have a centripetal acceleratio, a = v2/r, where v is the speed of the moon and r is the radius of its orbit. but n v = d/t = 2 pr / T (T, usually called the period) is the time for the moon to revolve around the Earth. Thus a = 4 p2r / T2. Go to REFERENCES and find values for r and T. How does the value of the centripetal acceleration in part 2 compare with the value calculated in part 1?

See this applet

This conclusion, that the force that pulls things to Earth is the same force that keeps the moon in its orbit , is called the Newtonian Synthesis. No longer are there separate rules for heaven and Earth. Newton the introvert does not publish these thoughts because he has no real need to show off. The information comes to light when, at the behest of Edmund Halley, Newton published the Principia, the first physics book.
The law of universal gravitation looks like this F = G M
1 M2/d2

There is a problem with the units in this equation. The left side in modern terms would be measured in Newtons. The right side was more difficult because it is measured in kg2/ m2. Henry Cavendish was able to show using a very sensitive torsion balance that 1 kg2/m2 = 6.67x 10-11 N. Dividing both sides by kg2 and multiplying both sides by m2, we get 6.67 x 10-11 N m2/kg2 = 1. We shall rename the quantity on the left G - the Universal Gravitational Constant.

A carbonated beverage recently opened on the Earth undergoes a separation of matter that is caused by gravity (bubbles rise but water does not). What happens to the liquid and the gas if the mixture is aboard a space shuttle orbiting the Earth.

Satellite Motion

Planets around the sun
Combining the principle of universal gravitation with the concept of objects moving in circular paths leads us to some remarkable conclusions about the planets and about the technical hurdles that must be overcome to put satellites in orbit around the Earth.
Consider a planet moving about the Sun in a circular orbit. (Note that for the smaller planets close to the Sun, this is a very good approximation.) Go to Equations, either at this site or in the classroom. Find page 4, lines 4 & 5 and set the parts of the equations equal to each other .

 If planets move in (nearly) circular orbits, some force must be acting as a centripetal force. The only candidate available is gravity. See the Equations page, specifically page 4 Let us tidy up the mathematics The speed of an object can be determined by dividing the circumference of an orbit by the time it takes to travel that distance Substitute line 4 into line 3 Solve line 5 for the mass of the sun. Note that the term is nothing more than Kepler's law of periods From these few lines of algebra we learn

1. We can calculate the mass of the sun by observing a planet that orbits the sun.
2. By simple extension, we can calculate the mass of any planet observing a moon that orbits the planet.
3. The term is precisely Kepler's law of periods first set down in 1618.

Satellites around the Earth

We can adapt the reasoning presented above to consider a human-crafted satellite (as opposed to the moon) in orbit about the Earth. it can be shown from the reasoning above (can you do it?) that the orbital velocity for this satellite is Go to References to find the pertinent data then calculate the following
1. The orbital velocity (in m/s and mi/hr) of a satellite in orbit at the surface of the Earth.
2. Determine the period (time for one orbit) for this satellite.

in the orbital velocity of a satellite around the Earth is about five miles a second something like17,600 miles per hour. Scientists have known about that number since 1799 wherein Henry Cavendish determined the universal gravitational constant. How absolutely absurd it must have been to consider something traveling five miles a second when the fastest being on the planet was a racehorse. for the next 150 years, travel beyond the confines of the earth was little more than dream.

Velocities approaching those necessary for orbiting this planet became attainable after World War II when the Soviet Union and Western powers assimilated German rocket scientists into their military programs to begin to exploit advances made by the Germans in the V-2 rocket program. During the 1950s United States and the Soviet Union began a serious attempt at launching satellites to orbit the Earth. This competition between the two countries to reach a space first was called a space race and the early milestones were won by the Soviet Union. In October 1957, the Russians launched Sputnik I, a small-payload satellite which took its temperature and transmitted data to ground stations. The first craft launched by the United States to attain orbit was Vanguard 1 launched from Cape Canaveral in Florida in January 1958. In between 1958 and in 1961 the Russians launched the first dog in space, the first man in space, first woman in space John Glenn orbited the Earth three times in February 1961.

These early launches had scientific as well as political value on a planet caught up in a cold war. The first commercial application of satellite technology came in 1963 when the United States launched Telstar I, the first communications satellite. Telstar was placed in near-Earth orbit to serve as a relay link between NorthAmereica and Europe. The U.S. ground station was located in Andover Maine, near Bethel. But because Telstar was in near-Earth orbit, it was in proper send/receive position for only about 15 minutes every 90-minute orbit, a good first try but unacceptable by modern standards.

Syncom I launched in 1964 was placed in geosynchronous orbit above the equator. When properly placed, these satellites maintain a fixed position above some point on the equator and thus are always in position to send and receive transmissions. Let us calculate the speed and position of such a satellite.

 This is the equation for the orbital velocity of a satellite, as derived above. The speed of an object can be determined by dividing the circumference of an orbit by the time it takes to travel that distance. In this case let T = 24 hours Set cell 1 = cell 2 Square both sides Solve for R R calculates to be about 26,000 from Earth center, or about 22,000 miles above the surface.Any other placement is said to be a useless orbit for a communication satellite.

Here is an applet where you can adjust the launch velocity for a projectile causing it to travel further and further down range until it has become an Earth satellite. http://www.phys.virginia.edu/classes/109N/more_stuff/Applets/newt/newtmtn.html

a) How large must the launch velocity be to cause the satellite wanna-be to strike Earth at points A or B?
b) What must be the minimum velocity of projection to cause the satellite to orbit the Earth?
 http://ericir.syr.edu/Projects/Newton/12/Lessons/gravity.html http://ericir.syr.edu/Projects/Newton/11/blckhole.html

On-line - stacking blocks
http://www.phy.ntnu.edu.tw/java/block/block.html

Go to problems at U Oregon
http://www.zebu.uoregon.edu/~probs/mech/grav.html