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34<br />

C h A p T E R 3<br />

The Gravitational Interaction<br />

Gravitational<br />

Constant<br />

A number relating <strong>the</strong><br />

strength of <strong>the</strong> gravitational<br />

force to <strong>the</strong> masses<br />

being attracted <strong>and</strong> <strong>the</strong>ir<br />

distance apart.<br />

henry Cavendish<br />

British scientist known for his<br />

work with hydrogen <strong>and</strong> his<br />

experiment that measured<br />

<strong>the</strong> gravitational force<br />

between two masses in<br />

order to calculate <strong>the</strong><br />

density of <strong>the</strong> Earth.<br />

MIRROR<br />

o<strong>the</strong>r object by a long- range gravitational<br />

interaction that obeys Newton’s Third<br />

Law. The strength of <strong>the</strong> attractive force,<br />

F, varies with <strong>the</strong> masses, M <strong>and</strong> m, of <strong>the</strong><br />

two objects <strong>and</strong> <strong>the</strong> distance, d, between<br />

<strong>the</strong>ir centers according to <strong>the</strong> relationship<br />

F = GmM/d 2<br />

The number G that appears in <strong>the</strong> equation<br />

is <strong>the</strong> gravitational constant. G relates <strong>the</strong><br />

amount of mass to <strong>the</strong> strength of <strong>the</strong> force. In<br />

Newton’s day no one knew <strong>the</strong> value of G. It<br />

can only be found through experiment <strong>and</strong> is<br />

so small, 6.67 ¥10 –11 in <strong>the</strong> metric system, that<br />

<strong>the</strong> gravitational force between two 100-kilogram<br />

balls placed 30 centimeters apart is about<br />

one-millionth of a pound. Only if one of <strong>the</strong><br />

interacting objects has a large mass, like Earth,<br />

does <strong>the</strong> force become appreciable.<br />

The first public test of Newton’s universal<br />

Law of Gravity (<strong>and</strong> his laws of motion as well)<br />

came when he used <strong>the</strong>m to successfully calculate<br />

<strong>the</strong> time <strong>and</strong> place of <strong>the</strong> return of a comet<br />

which <strong>the</strong> English astronomer, Sir Edmund<br />

Halley, suspected was orbiting <strong>the</strong> Sun. When<br />

“Halley’s” comet appeared just as Newton had<br />

predicted, <strong>the</strong> <strong>science</strong> of using ma<strong>the</strong>matics<br />

based on universal laws to know future motion<br />

was born.<br />

Using <strong>the</strong> heavens as a testing ground was<br />

successful. But one could still argue that gravity<br />

emanated only from <strong>the</strong> Sun <strong>and</strong> planets<br />

<strong>and</strong> was not present in ordinary objects, such<br />

as buildings or rocks. It was a leap of faith for<br />

LIGHT<br />

SOURCE<br />

SCALE<br />

figure 3.6<br />

A Cavendish balance. When <strong>the</strong> large spheres<br />

are in <strong>the</strong> position outlined by dashes, <strong>the</strong>y exert<br />

no measurable force on <strong>the</strong> smaller suspended<br />

spheres. When <strong>the</strong> larger spheres are rotated to<br />

<strong>the</strong> position shown, <strong>the</strong>ir gravity attracts <strong>the</strong><br />

suspended spheres. The amount of attraction is<br />

measured by <strong>the</strong> light beam’s displacement<br />

along <strong>the</strong> scale.<br />

Newton to hypo<strong>the</strong>size, without being able at<br />

that time to prove, that a force of gravity universally<br />

exists between any two objects that have<br />

mass. This aspect of <strong>the</strong> law was confirmed 70<br />

years after Newton’s death by Henry Cavendish<br />

(1731–1810), who developed a method of<br />

measuring <strong>the</strong> minute gravitational attraction<br />

between such ordinary objects as metal balls.<br />

In Newton’s day no one knew what <strong>the</strong><br />

mass of Earth was. So <strong>the</strong>re were two unknown<br />

values, G <strong>and</strong> M, in any formula expressing <strong>the</strong><br />

force of Earth’s gravity. An experiment was<br />

needed to measure <strong>the</strong> force of gravity between<br />

two known masses so that <strong>the</strong> value of G could<br />

be determined. (Then <strong>the</strong> mass of Earth could<br />

be found.) In <strong>the</strong> late 1700s <strong>the</strong> shy, eccentric<br />

Cavendish did just that (see Figure 3.6).<br />

Cavendish used two small gold or platinum<br />

spheres mounted on opposite ends of a lightweight<br />

metal bar suspended in <strong>the</strong> middle by a<br />

very fine wire. The wire had a mirror mounted<br />

in <strong>the</strong> middle of it. A focused light beam<br />

reflected off <strong>the</strong> mirror <strong>and</strong> onto a scale across<br />

<strong>the</strong> room. As two large lead spheres were<br />

brought near <strong>the</strong> small spheres, <strong>the</strong> gravitational<br />

attraction between <strong>the</strong> small <strong>and</strong> large spheres<br />

twisted <strong>the</strong> wire just enough to move <strong>the</strong> light<br />

spot on <strong>the</strong> scale. In this way <strong>the</strong> force required<br />

to twist <strong>the</strong> wire was determined, <strong>the</strong> force<br />

between <strong>the</strong> large <strong>and</strong> small spheres was<br />

inferred, <strong>and</strong> <strong>the</strong> Universal Law of Gravitation<br />

was used to calculate G from G = Fd 2 /Mm.<br />

3–7 ACCELERATION REVISITEd<br />

There is a final point regarding <strong>the</strong> value<br />

of <strong>the</strong> acceleration of gravity, g, that needs to<br />

be cleared up. At <strong>the</strong> beginning of <strong>the</strong> <strong>chapter</strong><br />

we found that g did not change for a rock as<br />

it fell off a cliff. Every second its velocity<br />

increased by <strong>the</strong> same amount. From this we<br />

concluded <strong>the</strong> force on <strong>the</strong> rock was <strong>the</strong> same<br />

at <strong>the</strong> top of <strong>the</strong> cliff as at <strong>the</strong> bottom. But <strong>the</strong><br />

Law of Gravity clearly says <strong>the</strong> force of gravity<br />

gets stronger as <strong>the</strong> distance between objects<br />

decreases. Therefore g should be larger at <strong>the</strong><br />

bottom of <strong>the</strong> cliff than at <strong>the</strong> top!<br />

As it turns out, <strong>the</strong> force of gravity is<br />

stronger at <strong>the</strong> base of <strong>the</strong> cliff than at <strong>the</strong> top<br />

by <strong>the</strong> amount that <strong>the</strong> Law of Gravity predicts,<br />

but <strong>the</strong> effect is very slight. A beach at sea level<br />

is 6,378 km from Earth’s center. The top of a

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