Emanresu said:
But the reason I say that it goes into the same change in velocity is because it is constant acceleration caused by a constant force caused by a constant supply of energy.
I am burning fuel (releasing energy) at a constant rate in time to create a constant force and yet my rocket is not gaining energy at a constant rate in time. So what is happening in terms of conservation of energy ?
Why do you say this? Where is this "increase" in energy?
Let's say the fuel burns an amount of E per unit time.
Now let's do this 2 ways, via a simple conservation of energy and then via the amount of work done by the force being applied. Already we can see that
E = \Delta(KE)
which means that
E = 1/2 m(v_f^2 - v_i^2)
This E is a constant throughout, and so is the difference in the square of the velocity, NOT the difference in velocity. That's why you were making a mistake when you comparing the change in going from 0-5 m/s versus 10-15 m/s. This is NOT the fundamental quantity that you should be dealing.
Now, let's consider this via the force applied, since you were worried about the acceleration. Rewriting the first equation using work done
E = \int{F ds}
where ds is the differential displacement. Now, it has already been pointed out that we can write F as
F = ma = m dv/dt = m \frac{dv}{ds} \frac{ds}{dt} = m \frac{dv}{ds} v
This means that
E = m\int{v dv}
Guess what? When you do the integral, you end up with the exact same expression as the one I got using conservation of energy.
Again, there's gain or change in energy over the unit time period in which E is burned from the fuel. What you are confusing with here is the insistance that \Delta(v) be constant, where as in actuality, it is \Delta(v^2), which is a direct result from the conservation of energy.
So there are no energy being created nor loss here.
Zz.