Suppose for example that we have a rocket loaded with fuel, initially at rest in our frame of reference. When we start the engines, some of the fuel is ejected at high speed from the exhaust of the rocket. The exhausted fuel now has some linear momentum in our reference frame. The total linear momentum before the firing of the engines was zero. Since it is conserved, the total must remain zero. This means that the momentum of the fuel in the backward direction must be exactly balanced by the momentum of the rocket in the forward direction. Therefore the rocket moves forward.
Linear momentum is the product of mass times velocity. If we know the mass and speed of the exhausting fuel at any instant, knowing that the product of those numbers must equal the mass of the rocket plus its remaining fuel, times the rocket's speed you could calculate the speed of the rocket without knowing anything about the forces involved, just from the conservation of linear momentum. Of course we could calculate the force experienced by the rocket once we know how its speed changes over time by applying Newton's second law that force equals mass times acceleration.
These ideas are easy to express in words as I have done here, but the mathematics in the case of real rockets gets very messy. You can probably find some examples in your text book, set up to be easily solved.
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