user079622 said:
Basically my question is; does our rockets/probes in space, whenever engine is working they accelerate?
The engine only accelerates the rocket when it has fuel.
So, the maximum speed of a rocket depends upon (1) the amount of fuel relative to the payload, and (2) the velocity with which the engine ejects mass from the rocket (which, in turn, depends upon the design and efficiency of the engine and the energy density of the fuel).
All chemical fuels have energy densities of the same order of magnitude. Nuclear fuel is much, much more energy dense, so a comparable sized rocket with nuclear fuel can reach much higher speeds than a chemical fuel rocket, even though a rocket with nuclear fuel needs a bigger payload to shield the payload from the radiation of the nuclear blasts that move the rocket.
The tricky thing about a rocket is that the amount of fuel is not independent of the amount of fuel you need to reach a certain velocity (i.e. speed).
This is because until you burn it, your engine needs to push not only the rocket's payload but also the fuel you haven't used yet.
In the image above of a real historical rocket using chemical rocket fuels that was used to go to the moon, only the area circled in red is the payload. Everything else in the image is fuel (and temporary engines to use it until that segment's fuel is used up) that gets disposed of segment by segment as the fuel from that segment (also called a "stage" of the rocket) is used up.
As Wikipedia explains:
The
classical rocket equation, or
ideal rocket equation is a mathematical equation that describes the motion of vehicles that follow the basic principle of a
rocket: a device that can apply acceleration to itself using
thrust by expelling part of its mass with high
velocity can thereby move due to the
conservation of momentum. . . . The necessary wet mass grows exponentially with the desired delta-v.
The equation is as follows:
Where "e" is
Euler's number (a
mathematical constant equal to 2.71828 . . . .).
So, the faster you want your rocket to go, the bigger the percentage of the rocket that is used for fuel must be.
The only loopholes that can be used to reach a speed greater than the speed allowed by the ideal rocket equation involve using source of energy to achieve higher speed other than thrust from the rocket engine derived from carried fuel.
In practice, the two main exceptions to the ideal rocket equations are (1) to gain speed with a
gravitational slingshot effect, and (2) to use a beam of energy like a laser (or solar energy) to transfer energy to the rocket that doesn't come from its own carried fuel. The laser allows for significantly higher acceleration than relying on solar energy (a design called a "
solar sail"), but is limited by the need to have a line of sight between the laser and the rocket and the need to keep the laser beam perfectly focused over a long distance. But both methods accelerate the rocket above its maximum speed using carried fuel alone.
An artist's impression of a solar sail.