Question #a288d

1 Answer
Jul 17, 2015

The answer is (c) decreases.

Explanation:

The idea behind this problem is that Earth's roration produces a centripetal acceleration, which is directed towards the center of rotation, that reduces the gravitational acceleration, gg.

This centripetal acceleration is defined by the equation

a = omega * r^2a=ωr2, where

omegaω - the angular velocity of the Earth;
rr - the radius of the Earth.

The force that creates this centripetal acceleration is called the centripetal force and is pointed towards the center of ration as well.

F_"centripetal" = m * a = m * omega * r^2Fcentripetal=ma=mωr2

Now, an object that is in a rotating reference frame, i.e. a reference frame that is rotating with the system, will be acted upon by the centrifugal force.

This "force" (it is not a force per se) points outwards from the center of rotation and actually replaces the centripetal force.

F_"centrifugal" = m * omega * r^2Fcentrifugal=mωr2

![http://www.calctool.org/CALC/phys/newtonian/centrifugal](useruploads.socratic.org)

This means that, for a person that's rotating at the equator, this centifugal force will actually oppose gravity.

This means that the weight of the person at the equator will actually be

cancel(m) * g_(eq) = cancel(m) * g - cancel(m) * omega * r^2

For future reference, g_(eq) is actually called the acceleration due to gravity at the equator.

As you can see, the magnitude of g_(eq) depends on omega, which is the angular speed of rotation.

This bigger omega gets, the smaller g_(eq) will become, since you're subtrating an increasingly bigger number, omega * r^2, from g.

As a conclusion, the faster the Earth spins, the lower g_(eq) will be, which in turn means that a person's weight decreases.