Answer 4: Let’s take a look at Newton’s law of universal gravitation to help answer your question. Newton’s law states that the force (F) enacted on two bodies interacting with each other due to gravity is the product of the gravitational constant (G), the masses of the two bodies (m1 and m2) and the inverse of the distance squared between their center of mass (1/r2). The complete equation is: F = G*m1*m2/r2. If we take out the mass of the variable body (i.e. keep the mass of the moon in the equation), the equation reduces to the acceleration (a) due to the gravitational force of the remaining body. You can verify that the acceleration at the surface of the Earth should be 9.8 m/s2 (one G) by using these numbers (from hypertextbook.com; make sure units correctly cancel out!): G = 6.7X10-11 m3/kg/s m_earth = 6X1024 kg r = (diameter_earth)/2 = (12800 km) / 2 = 6400 km = 6.4X106 m Thus, a = G*m_earth/r2 = 9.81 m/s2 (correct!) So, now we can calculate the acceleration of an object 100,000 km from the surface of the moon. We need to make sure to add the distance from the center of the moon to this 100,000 km (numbers again from hypertextbook.com): m_moon = 7.5X1022 kg r = 100,000 km + (diameter_moon)/2 = 100,000 km + (3480 km)/2 = 1.02X108 m Thus, a = G*m_moon/r2 = 4.8X10-4 m/s2 The results should be expected; we are looking at the gravitational effects of something that is very, very far away from the moon (about 1/4 the distance from the Earth to the moon). But while the numbers seem very small, they are not negligible. The small shifts in gravitational force are indeed enough to cause changes on Earth such as the rise and fall of tides due to the moon (and Sun). |