Perhaps an example may help: Filling a long line up to a receiver vessel that is a long distance away and at a higher elevation than the pump. At the other end of the line is a flow meter that consists of a meter reading the pressure drop across an orifice plate. After that, there is a control valve that is attempting to hold constant flow in the line. The vessel is vented to flare so that no gas pressure builds up ahead of the liquid. We start with a vacant system and start up a large circulating pump. With no back pressure, the pump runs out to the end of the curve which may be twice the normal flow rate. The flow meter at the other end does not register this flow because only gas is passing through the orifice plate. An equivalent volume of gas does not produce much pressure drop as compared to water. Since the meter is sensing low flow, the control valve goes wide open attempting to reach set-point. The velocity of the water coming up the pipe is twice the normal velocity since the pump is running out to the end of the curve. When the water reaches the orifice plate, there is a sudden increase in pressure drop across the orifice plate. But, the column of water coming up the pipe cannot slow down instantly. In fact, the pressure wave coming back from the orifice plate can only travel at the speed of sound. So, the column of water keeps moving forward at the original high velocity until the pressure pulse gets back to the pump to push it back up on the curve. Since water is basically incompressible, an incredibly high pressure may be achieved before the pump flow drops off. The longer the line, the higher this pressure may build since it will take even longer for the pressure wave to travel back to the pump. In addition to the immediate pressure wave, when the flow meter senses the high flow, the control valve will close to try and achieve set-point. The rapidly closing valve could produce another pressure wave that would also have to travel back to the pump before the pump flow could be reduced. The resulting pressure spikes could be many times greater than the shut-off head capability of the pump. It could blow the line apart. This same event could happen if there was a heat exchanger, filter element, pinched valve, or reducer in the line.
You have never described the main pumps in your system. The problem with operation at the end of curve depends on the pump. Another example may help. Our largest water pump is a 10 stage barrel pump. All 10 impellers are in series, oriented in one direction. In order to counter the extremely high thrust that would result from these 10 impellers, there is a balance piston on the discharge end. The balance piston uses a pressure differential between suction pressure on one side and discharge pressure on the other side to counter the thrust of all 10 impellers. This particular pump normally runs with about 3600 psi discharge pressure. If we were to operate the pump with a wide open discharge line and no back pressure, there would be no discharge pressure against the high pressure side of the balance piston. Operating in this mode, the individual impellers would also be producing less thrust. But, there could still be many thousands of pounds of thrust produced by the impellers that the balance piston could not counter. Running this way for even 10 seconds could result in a thrust bearing failure.
Cavitation could be viewed as a long term reliability issue. But, water is the most destructive fluid for cavitation. Running in hard cavitation for 10 seconds at each start-up could result in cumulative damage to the first stage impeller. Depending on how often the process is started, this cumulative damage could be very significant. Also, while running in hard cavitation, the shaft deflection would be greater. I would expect an increase in bearing and mechanical seal failures by running in this mode.
Johnny Pellin