There is say a satellite revolving around the earth at a quite a
good height h. Say now it suddenly stops and falls down to earth.In
what time will it come down?
(This is just my own made up question so the ending expression for
time may include some terms i have not introduced here)
I have tried a lot though if you see i got stuck on just one
complication,
we know that g at a height h is->
gh=g[R/(R+h)]2
Since g here is varying i am not able to put it in any of the
kinematic equations.
love arun
Glancing quickly at your equation it looks unfamiliar, though it
could well be right. I wouldn't use it though, when we know:
F=Gm1m2/r2 (Newton's law of
gravitation).
F=ma (Newton's second law, constant mass)
Þ a=Gm/r2 (where m is
the mass of the Earth here)
\ d2r/dt2 =
Gm/r2
and now solve this differential equation to relate r and t (you
will need to set boundary conditions).
Jim,
i think you are overlooking some facts.Practically speaking we have
here another force to reckon with that is drag force of the
air. Due to this force,the body achieves certain maximum
velocity called the terminal velocity.After achieving this
velocity,the body does not accelerate.
There are again much more complications regarding terminal velocity
(which should vary quite significantly in this particular
problem).All of this is too long to write down right now.
I hope you get the feel of my problem.
love arun
Well we know that the drag force is crudely proportional to the velocity squared, so we can simply take account of that fact in the differential equation...
I seem to end up with the differential equation:
r'' + k(r')2 = Gm/r2
where acceleration, a = r'' and velocity v = r'
This looks like a killer equation to solve so the best thing to do
would be to define the initial conditions and solve it numerically.
Ah, the bane of all physicists, I did indeed forget air
resistence. But even if we assume it proportional to speed squared
(this is true at very high speeds, at low speeds it is proportional
to speed, and in practice it is somewhere in between! :-P) we are
still forgeting something. As you might expect, air resistance is
dependant upon (in fact proportional to if I remember correctly)
the density of the fluid it is travelling through. But Arun said "a
satellite revolving around the earth at a quite a good height," so
we are talking about starting in a low (or even zero) density
atmosphere, and this varies as we come closer to the earth. I will
look on the internet for details of the variation, but in all
honesty I'm not optimistic.
Jim
I have just read that atmospheric pressure varies exponentially
with height. I leave it to you to solve the resulting differential
equation (!)

Jim
Oops, that first minus should be a plus (since (negative)
acceleration due to air resistence and acceleration due to gravity
act in opposite directions).
Jim
It does not end here my friends.
Point No.1->
the air resistance not only drags the body up but also must be
setting up various types of frictional forces which must be taking
place at atomic level.These forces tend to deform or even sometimes
burn the object.(this observation is purely my opinion so it is
open for criticism)
Point No. 2->
What about terminal velocity?
In my opinion,while solving this problem,we should actually divide
the path of falling satellite into 3 different zones---1>low
pressure 2>moderate pressure 3>high pressure.According to
me,the body must attain three different terminal velocities while
traversing through its path.As i already said above,the body
doesn't accelerate after it has reached terminal velocity.Hence,the
body travels with zero acceleration during three parts of its
path.
If i am wrong at some points,please do correct me.Actually i am
trying to solve this problem for nearly a year or so and the points
i have mentioned above were certain things i could not
rectify.
love arun
1. You are right, if the air resistance deforms the body it will
effect the value of the air resistance (and also on the mass,
affecting other parts of the equation). If there are big solar
panels or something sticking out this could have quite an effect,
but if the body is quite centralised hopefully there will be little
difference.
2. I disagree (IMHO). Of course a body will never QUITE reach
terminal velocity, but will come closer and closer to reaching it.
Since this is a natural reflection of the physics involved, I think
the equation when solved (not that I can do it) will account for
that.
Does anyone have any idea how to solve the equation (a, b and m are
constants)? I don't even know how to do it numerically. The plus
and minuses have changed again, it should definitely be right this
time J.

Jim
I think I have an idea of how to solve it, but I don't think
that it will have a closed form solution. First, write the equation
as
d2r/dt2+a×ebr(dr/dt)2=c/r
2
not really caring at the moment what a,b, and c are.
Note that this is equivalent to
d/dt(exp(aebr/b)dr/dt)=c×exp(aebr/b)/r
2
putting exp(aebr/b)dr/dt=x, we are given
dx/dt=(dx/dr)×(dr/dt)=c×exp(aebr/b)/r2
multiplying by exp(aebr/b), we get
x×dx=(c×exp(2aebr/b)/r2)dr
we can now integrate both sides, however, I'm not sure the the RHS
has an algebraic integral.
Brad
This is the same integral you have posted under the topic
COMPLEX INTEGRAL, isn't it?
I don't know why but i have feeling that RHS might involve the term
Ei(x) and g [Euler's constant]
If it does involve such terms,we will have then to reevaluate the
entire thing.
love arun
Well,
anybody lucky to have got the solution to that differential
equation?
love arun