UMath1 said:
Shouldn'tit have a downward acceleration? If you fire a bullet horizontally, it's x-velocity is constant but due to acceleration in the y-direction it acquires velocity in the y-direction and curves in a parabolic path. Similarly, when a satellite is launched it curves. So isn't it accelerating in the y-direction like the bullet? The only difference that for some reason for every gain in y-velocity the satellite lose x-velocity. I don't understand the concept behind how this works.
In your first example you are assuming that gravity always pulls in the y direction as in the top left diagram in the image below. However, this is only an approximation that works if we are dealing with rather small projectile velocities such that the distance traveled in the x direction is small compared to the size of the Earth.
The more accurate description of what happens, and the one you need to consider with satellites is the upper right diagram. Here, when the projectile starts, the pull of gravity is in purely the y direction. However, as it moves in the x direction, gravity which always acts towards the center of the planet, starts to gain an m x direction component which acts on the x velocity of the projectile.
The bottom 2 diagrams demonstrates Newton's theorem of areas, which proves that an object responding to a centrally acting force will sweep out equal areas in equal times.
First consider an object traveling at a uniform velocity such that it travels from A to B in one second. in relation to point O it sweeps out the triangular area OAB in one second. 1 sec later it arrives at point C, having swept out triangle OBC. Since the two bases AB and BC and the altitude (the red line) of these triangles are equal, the areas of triangles OAB and OBC are equal.
Now assume that upon reaching B, the object is acted on by an instantaneous force acting along the BO line. The force is such that if, the object was at rest with respect to O, it would be given a velocity such that it would arrive at point D after 1 sec. It is not at rest however and has a BC velocity and the end result is a velocity that has the object arrive at E after 1 sec. Thus in one sec it sweeps out triangle OBE. Note that triangles OBC and OBE share 1 side OB and since the lines BD and CE are parallel, the two red lines are of equal length. If we take OB as the base of both triangles, the red lines are their altitudes, and triangles OBC and OBE are equal. Since we already showed that OAB and OBC are of equal areas, triangles OAB and OBE must also be of equal areas. Thus the object sweeps out an equal area both before and after being acting on the force towards O. If the object were acted on by a force in the direction of O at point E, the same argument as above shows that the triangle that it sweeps out in the next second will be equal in area to OBE and by extension, OAB.
By shortening the time periods between the applications of the force in the O direction we reach the limit of a constantly acting force pointing towards O. (just like gravity constantly acts towards the center of the Earth.) and show that the area swept out by a moving object subjected to such a centrally acting force would be an equal amount in equal times. An object traveling in a circle at a constant tangential speed also sweeps out an equal area in equal times, So it is no wonder that a satellite traveling at the right tangential speed would maintain a circular orbit.
Elliptical orbits are also possible, and they also sweep out equal areas in equal times, and they do so by varying tangential speed with varying distance.(technically, all closed orbits are elliptical, as circles are just a special case of an ellipse.) The limits for an elliptical orbit are that its lowest point cannot be lower than the surface of the object it is orbiting, and its speed cannot be so high that it escapes the planet completely.