Henry Cavendish used a torsion balance, a horizontal rod hung from a thin wire with small lead balls at each end, to measure the tiny gravitational pull between the small balls and a pair of much larger stationary lead balls placed nearby. The twist in the wire told him how strong that pull was, and because he knew every mass and distance involved, he could apply Newton's law of universal gravitation directly to work out the gravitational constant and, from it, the density of the Earth. It was the first time gravity between ordinary sized objects had been measured in a laboratory rather than inferred from the motion of planets, and it confirmed that Newton's law holds at that much smaller scale too. This description is adapted from Wikipedia contributors under CC BY-SA 4.0; changes were made. https://creativecommons.org/licenses/by-sa/4.0/
Facts
YearSourced to the subject's own account MethodSourced to the subject's own accountA torsion balance: a six-foot wooden rod horizontally suspended from a wire, with a lead sphere attached to each end, used to measure the gravitational attraction of nearby large masses. 1 Connections
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Source Henry Cavendish (Wikipedia)
Tests
Source Cavendish Experiment (Wikipedia)
Uses
Michell's torsion balance, inherited and modified by Henry Cavendish, is the instrument the Cavendish experiment is built around.
Source Torsion Balance (Wikipedia)
Sources
1. Cavendish Experiment (Wikipedia)
WikipediaIntroduction
The apparatus consisted of a torsion balance made of a six-foot (1.8 m) wooden rod horizontally suspended from a wire, with two 2-inch-diameter (51 mm), 1.61-pound (0.73 kg) lead spheres, one attached to each end.
In Group: Physics Experiments, Lead
was the first experiment to measure the force of gravity between masses in the laboratory and the first to yield accurate values for the gravitational constant
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WikipediaUses: Torsion Balance, Torsion balance sectionQuote, Uses: Torsion Balance, Torsion balance section
The torsion balance, also called torsion pendulum, is a scientific apparatus for measuring very weak forces, usually credited to Charles-Augustin de Coulomb, who invented it in 1777, but independently invented by John Michell sometime before 1783.
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