here, let me spell it out more explicitly:
please try to read this carefully, and if you find any genuine conceptual mistakes, address them explicitly.
the purpose of my original post was to attempt a feasibility assessment of the tugging solution.
1) If Earth's gravitational field magically disappeared, it would be easier to deflect an incoming asteroid.
2) If we calculate how much force would be required to deflect an incoming asteroid,
within a timelimit, and compare that to the force that a "small apollo sized tractor ship" could exert, and we do this
assuming no earth gravity,
and it turns out to be not enough, then we can safely say that if
there were earth gravity, then it would definitely not be enough.
stated another way: 2) if it's not feasible assuming no earth gravity, then it's certainly not feasible
with earth's gravity, as earth's gravity only makes the task
harder.
Do we agree up to this point?
3) If we assume no earth gravity, then I argue that you don't need polar coordinates (i'm not even sure what you'd do if you did want to incorporate earth's gravity, short of a computational simulation) - if you know how much you want to orthogonally displace the asteroid, and you know how much time you have to achieve this displacement, then you can calculate how much acceleration is required, using basic 2 dimensional kinematics. Furthermore, this is another leniency on the feasibility assessment since the calculations assume that the tugging force is being applied for the entire duration - so if it turns out not to be feasible with tugging for the whole duration, then it's certainly not feasible with tugging for only part of the duration.
I will now attempt to demonstrate 3):
In the first picture, we see the situation at time 1:
The black arrow going left indicates the movement of the asteroid - it is not accelerating forwards, and there is no force acting in this direction.
The blue arrow pointing upwards indicates the tugging force.
Notice that the direction of force is orthogonal to the direction that the asteroid is traveling.
Now this is our end goal:
The key point to note here is that the displacement D is
solely due to the orthogonally applied force seen in the first image.
If we know what D is, and we know the time we have to achieve this displacement, then we can calculate the orthogonal force required.
Now let's see how we apply this:
Let's say that our current technology gives us the ability to tug for 6 months. This includes being able to predict a collision at least 6 months in advance, and securing a ship to tug 6 months away from collision.
We thus have:
displacement (radius of earth, assuming it's on a collision course with earth's centre)
time
initial velocity along direction of displacement (0 m/s)
we can thus calculate the necessary acceleration.
If we have the mass of the asteroid, we can then calculate the necessary force to be applied over time.
We can then see how much force an apollo sized tractor craft is capable of exerting, and see if it meets our bill.
If it doesn't, then we can be sure that it wouldn't meet the bill if there were earth's gravity to consider.
That is all i'm trying to say here.