No one has mentioned the deceleration issue. If you could, hypothetically, increase delta-V - or your change in velocity, to whatever you wanted, then you still face the problem of slowing enough to enter the orbit. You would have to increase the amount of fuel you'd have to burn in the opposite direction to slow down.
I'm no rocket scientist. But I've read enough science fiction to play one on TV. I don't know that Delta-V is the right way to think about this anyway. Delta-V is dependent on the Gravity one is experiencing (its delta V, provided by positive Acceleration, in magnitude sufficient to counteract the negative acceleration of gravity, commonly give as -9.81 m/s^2). Delta-V represents the kinetic energy of the rocket, ($KE = \frac{1}{2}mv^2$) and momentum ($p=mv$), which must be sufficient to escape a gravitational well.
At the same time, delta-V does not exactly represent the theoretical change in velocity of the actual rocket. It's really a way of taking specific impulse and putting it in terms of the body a specific impulse is trying to effect. There is no specific delta-v that works to achieve this. Rockets are typically given strength in terms of specific impulse, which is more useful than this "delta-V" measure, which I've never seen used in this way before, and I think it might be inappropriate.
A rocket can achieve a given delta-v in a specific set of circumstances- but another in another set- the two most important determinants would be the gravity and of course payload (or better yet total rocket mass). Delta-V is just the change in velocity the rocket can achieve for a given gravity and mass.
$$\Delta v = \int_{t_0}^{t_1} \frac{|T(t)|}{m(t)} dt, $$
where $T(t)$ is the time-dependent thrust (assumed to be in the same direction as the velocity) and $m(t)$ is the time-dependent mass of the rocket as it uses up propellants.
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