The Ideas of Einstein's Theory : the Theory of Relativity in Simple Language

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footnote at the end of Chapter XV).
The description of the motion executed by a body under the action of force is further given by the Newtonian fundamental law of mechanics, which states : If no forces act on a body, that body will persist in a state of rest or of uniform rectilinear motion. If, however, a force act on it, acceleration wiU ensue. The direction of the acceleration will be parallel to the direction of the force, and the magnitude of the acceleration will be equal to the quotient
... of the force and the inertial mass of the body.
These laws were brought by Newton into the form of differential equations, and in point of fact, by their aid it is possible to calculate the motion carried out by a body under the action of given forces, or vice versa, to calculate the forces necessary to impart a certain state of motion to a body. How great the efl&ciency of this theory was, is shown by the history of the dis- covery of the planet Neptune — a discovery which is looked upon with full justification as one of the greatest triimiphs of human science, The French astronomer Levenier had observed that the combined forces of the hitherto known planets did not suffice to fully explain the orbit of the planet Uranus.


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