Mohammad Ishmas said:
well let us say that this system is being pulled from 625 kg block with the data given below
I notice that you have not given any data below. So I will harvest the data from up-thread.
We begin with blocks of 625, 200, 100, 50 and 25 kg arranged in a row from left to right on a frictionless surface, all connected with ideal massless cords.
We apply a leftward force of 62,500 N on the 625 kg block. We are invited to imagine that this is from a rocket
nozzle on that block. The nozzle is supplied with 12.5 kg/s of liquid propellant which is expelled with a relative velocity of 5000 m/s rightward.
The propellant is supplied in turn from the smaller blocks, starting at the right and working left. The blocks are pure propellant. Any tank is negligibly massive. Once the propellant in a block is exhausted, the block itself is discarded.
Consider the situation after 5 seconds has elapsed.
a) What is the acceleration of the assembly at this point?
b) What is the tension in the cord connecting the 625 kg block to the 200 kg block behind it?
I would analyze the problem by first calculating the system state at 5 seconds into the scenario. The trailing 25 kg tank would have been exhausted in the first two seconds. It will have been discarded and is now irrelevant. The 50 kg tank will have lost 37.5 kg of its initial mass. 12.5 kg remains.
So we have 625 + 200 + 100 + 12.5 kg = 937.5 kg total assembly mass at this time.
This assembly is subject to a net external force of 62,500 N.
Assuming that the assembly moves rigidly (as it obviously should) this means that it is accelerating at a rate of ##a = \frac{f}{m_\text{tot}} = \frac{62500}{937.5} \approx 66.7## m/sec
2
[Since gravity is not a factor, we will not be adjusting the acceleration to 56.7 m/sec
2]
Ignoring the 625 kg block in front, the mass of the remainder of the assembly is currently 200 + 100 +
50 + 12.5 = 312.5 kg. This assembly is accelerating leftward at approximately 66.7 m/sec
2. So it must be subject to a leftward net force of ##f_\text{net} = m_\text{tail} a \approx 312.5 \times 66.7 = 20833## N.
Naively, this is the tension in the cord between the 625 kg and 200 kg blocks: about 20,833 N.
If I've not muffed the calculation. [Edit: One muff corrected. I counted the 50 kg block when I should not have].
However, there is a momentum flow that we have not accounted for.
We are piping liquid propellant forward from the 12.5 kg (remaining) tank to the 625 kg block where the rocket nozzle is attached.
If the pipe is narrow, the velocity of propellant in the pipe times the 12.5 kg/sec flow rate may amount to a significant force. This would be a retarding force on the trailing block and a propulsive force on the leading block. The tension in the cord[s] would need to increase to reflect this.
If the pipe is wide and long, the mass of propellant in the pipe may be significant. This messes up our accounting for the mass of the various assembly bits at any point in time -- where do we count the mass of the propellant in the pipe?
So let us assume that the whole assembly is short and the pipe is wide so that the mass and momentum transfer from the unburned propellant in the pipeline may both be safely neglected.