7. Isaac Newton was the first person to correctly explain the twice-daily occurence of high and low tides. This happens because gravity is a force that depends on distance. Thus, the part of the Earth closest to the Moon (position 1 in Fig. 1) feels a stronger pull than the diametrically opposite part (position 2) which is the farthest from the Moon. The magnitude of the gravitational force between any two masses is given by where a is a constant that contains the two masses and d is the distance between the object feeling the force and the centre of the object exerting the force. Let R be distance from the centre of the Moon to the centre of the Earth and Rg be the radius of the Earth (see Fig. 1). Compute the tidal force using Fide 0 2. where 1,2 are the positions described above (red dots in the figure). To do this, let ar represent RE/R which is much smaller than 1 since R << R. Then using the Maclaurin series for d2 and d₂2 in Eq. (1) obtain the first non-zero term for the Fride as a series in a multiplied by constants. Finally, substitute x = RE/R into your expression to find that the tidal force depends on the inverse of the cube of R. RE 1 F1-F20 • (-a) R Figure 1: The Earth-Moon system (not to scale). Rg is the radius of the Earth and R is the Earth-Moon distance measured from the centres.
7. Isaac Newton was the first person to correctly explain the twice-daily occurence of high and low tides. This happens because gravity is a force that depends on distance. Thus, the part of the Earth closest to the Moon (position 1 in Fig. 1) feels a stronger pull than the diametrically opposite part (position 2) which is the farthest from the Moon. The magnitude of the gravitational force between any two masses is given by where a is a constant that contains the two masses and d is the distance between the object feeling the force and the centre of the object exerting the force. Let R be distance from the centre of the Moon to the centre of the Earth and Rg be the radius of the Earth (see Fig. 1). Compute the tidal force using Fide 0 2. where 1,2 are the positions described above (red dots in the figure). To do this, let ar represent RE/R which is much smaller than 1 since R << R. Then using the Maclaurin series for d2 and d₂2 in Eq. (1) obtain the first non-zero term for the Fride as a series in a multiplied by constants. Finally, substitute x = RE/R into your expression to find that the tidal force depends on the inverse of the cube of R. RE 1 F1-F20 • (-a) R Figure 1: The Earth-Moon system (not to scale). Rg is the radius of the Earth and R is the Earth-Moon distance measured from the centres.
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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