Gravitational force on objects

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When a feather and a rock are dropped simultaneously, the rock hits the ground first due to air resistance affecting the feather, not because of a difference in gravitational force. Both objects experience the same gravitational acceleration, but the feather's motion is hindered by air resistance, which is negligible for the rock. The equations of motion, such as v = gt and v = √(2gh), indicate that the velocity of falling objects is independent of their mass when air resistance is not considered. The conservation of energy principle confirms that the impact velocity is determined solely by the height from which they fall, regardless of mass. Therefore, in a vacuum, both objects would fall at the same rate and hit the ground simultaneously.
CAF123
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If I take a feather and a rock and drop them at the same time, because of the effect of the gravitational force, we know that the rock will hit the ground first. (The rock experiences a larger gravitational force).

My question is if these objects are dropped at the same time and vertically, then the velocity can be described as v = gt, for both objects. Therefore, at t = 1, v = 9.81 m s^{-1} and at t = 2, v = 19.6 m s^{-1}. However, i find it difficult to believe the feather will have this velocity. So how does the differences in gravitational force be accounted for in this equation?

Many thanks
 
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CAF123 said:
If I take a feather and a rock and drop them at the same time, because of the effect of the gravitational force, we know that the rock will hit the ground first. (The rock experiences a larger gravitational force).
The reason that the rock hits first is not because of its greater gravitational force. If only gravity acted, then both would have the same acceleration = g. But other forces are involved, in particular air resistance. Take away the air and the feather and rock will fall together.
 
I see, many thanks.
So essentially the formula only works when considering zero air resistance
 
yes and no...

Just before an object is dropped it has some energy let's call it Estart where

Estart = PEstart + KEstart

Since it's stationary KEstart = 0 so

Estart = PEstart = mgh

When it hits the ground it has some energy, let's call it Eend then

Eend = PEend + KEend

but PEend = 0 so

Eend = KEend = 0.5mv2

If we assume there is no air resistance to be overcome (or any other way for energy to leave the system) then the law of Conservation of Energy says

Estart = Eend

or

mgh = 0.5mv2

Notice how the mass cancels and the velocity of impact is independant of mass

v = SQRT(2gh)
 
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And if it takes t seconds to cover this distance h, either v = gt or v = \sqrt{2gh} can be used to determine this impact velocity, I presume?
 
CAF123 said:
v = \sqrt{2gh} can be used to determine this impact velocity, I presume?

That's what i said.
 
you have two objects of mass M and m, with M>m .
if you let them fall, you get from Newton's 2nd law:
M a1= - M g
m a2= - m g
from that you see immediately that a1=a2
which means the speed of the mass M will change by the same amount in the same time interval as will the speed of mass m.

The mass of the falling object, does not appear in your motion equations. It doesn't affect it.
Even if I didn't use the "static model", that the grav force is mg, but used the force:
F= G M' m /r (M':Earth's Mass)
the masses of the falling objects would again drop out.
Of course that is not obvious, it comes thanks to the equivalence principle, which says that the mass that appears in ma, and the mass that appears in m* (GM'/r) is the same
m=m*
 
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