A turbine is designed to work (efficiently) at a specific flow rate. Therefore, it shouldn't vary much. This is a plot defining turbine characteristics:
In green, you have the mass flow plotted against the pressure ratio for different corrected values of rpm (ranging from 80 000 to 180 000 rpm). In orange, you have the turbine efficiency plotted against the pressure ratio for the same rpm values.
Note that at high rpm, the mass flow is pretty constant across the pressure ratio range. That is because the flow is choked. Note also that maximum efficiency is when the flow is at high rpm and high pressure ratio (i.e. when the flow is choked).
One would only consider the points where the efficiency is maximum for each rpm. If you plot only the mass flow values corresponding to their respective maximum efficiency for their rpm, you will get something looking like this:
Here,
NF is the maximum allowable rpm. So near a pressure ratio of 1.4, the rpm stay constant (for example, like using solely the 160 000 rpm line from the previous plot for all points above that pressure ratio threshold). You can see that for take-off, cruise or climb, the mass flow is relatively identical, i.e. the flow is choked. The only exception is idling where a lower rpm is used to reduce friction losses for less fuel consumption (and probably lower noise level too).
The lower power settings are set by using less fuel, which will reduce the pressure ratio and you can find the corresponding mass flow on the plot. But, because of the lower efficiency, a turbine is not usually used that way in its normal use.