No, especially not for the conditions you stated.
Even if we consider that "same exact ariplane" will not melt away at Mach 2 or 5, different phenomena start to appear at such speeds.
Let's restrict speeds to below about Mach 0.5 for now. At such speeds, compressibility of air does not affect characteristics significantly, and things become easier. Still, drag will depend on how exactly the airplane is built.
Most aerodynamic forces at such speeds, including drag, are proportional to dynamic pressure:
$$q = \frac{\rho V^2}{2}$$
That is, linearly proportional to air density and to square of speed.
Now, drag consists of two parts: one related to lift, called induced drag, and everything else, often called parasitic drag. This parasitic drag, at such low speeds, will indeed change proportional to $q$,1 and can be calculated easily using the standard atmosphere table you found.
But not so with induced drag. Your lift will also change with $q$, and if you want to fly level, you don't want that. So you aim to have the same lift. You do it by adjusting the angle of attack. But by doing that, you change the "aerodynamic efficiency" of the airplane: that is, you change induced drag disproportionally. Normally, there is one "best" angle of attack, and if you move away from it, you'll have more induced drag even for the same lift. How much more? This entirely depends on how the wing and the entire airplane is designed.
You can find conditions where $q$ will be the same: you can fly higher (=> lower density) and faster, and come up with the same dynamic pressure. Pilots will see it as the same indicated airspeed (IAS). In such conditions, you will fly at the same angle of attack, and drag will be the same.2
So, in general, some of the drag will change predictably in a more or less universal manner, and some will depend on the airplane. And this is for the trivial case of low speeds.
Now enter compressibility (and other) effects, and things get much more complicated. Even the parasitic drag will change non-linearly; it will acquire a component called wave drag, which depends not on $q$ but on the Mach number - and on the actual shape of the airplane. Some airplanes will not see much up to M0.8 or even more, some will suffer at 0.6. The effect is most complicated at transonic speeds; at high supersonic speeds, shape starts to matter less. Furthermore, the way lift is generated also changes, which may produce extra drag (see e.g. trim drag).
So, your best bet is to get approximate data for some "typical" airplane. Concorde is a good candidate: it has some published data regarding its efficiency at sub- and supersonic speeds.
1 To the first level of approximation: there are still some fundamental effects that change, but we are doing back-of-an-envelope calculations.
2 Note though that on a practical level it will still affect the "extra energy needed". First, this energy comes from an engine, and its efficiency changes not only with $q$. Normally, it becomes more efficient in colder air (i.e. higher). Second, you'll reach the destination faster when flying higher at the same $q$ (IAS) and thus at about the same power setting (yet, on the other hand, having spent some energy climbing).