Control Systems Engineering : Masons Gain

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SUMMARY

The discussion centers on the application of Mason's Gain Formula in Control Systems Engineering, specifically regarding the steady-state error and block diagram representation. The user initially struggled with the dimensional consistency of their equations and the relationship between the rate of change of height (dh/dt) and the inflow and outflow rates (qin and qout). After correcting their equations and understanding the significance of the tank's area, they successfully derived the loop gain as (c_1 - c_2)/as, leading to a clearer understanding of signal flow graphs and Mason's formula.

PREREQUISITES
  • Understanding of Mason's Gain Formula in control systems
  • Knowledge of block diagram representation in control theory
  • Familiarity with dimensional analysis in equations
  • Concept of steady-state conditions in dynamic systems
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  • Study the derivation and application of Mason's Gain Formula in various control systems
  • Learn about dimensional consistency in physical equations and its importance
  • Explore the relationship between flow rates and tank height in fluid dynamics
  • Investigate advanced block diagram techniques and signal flow graph analysis
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Control systems engineers, students studying control theory, and anyone interested in mastering Mason's Gain Formula and its applications in dynamic systems.

BartlebyS
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Homework Statement



Here is the system I am looking at

image.jpg


Homework Equations



So I worked out a formula for the steady state error and put it in a form similar to masons gain formula

image.jpg


The Attempt at a Solution



But when I try and draw a block diagram and work out e I get confused by forward path and loop gain. It's not a question I have been asked, I am just playing, perhaps I cannot apply masons gain to my drawing? Or my drawing is wrong?

image.jpg
 
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Your equations are not correct. For one thing, they are not dimensionally consistent: dh/dt = qin - qout has different dimensions on each side. q has dimension L^3 whereas dh/dt has dimension LT^(-1). L = length, T = time.

Your block diagram is good up to the point qin but then falls apart. Correct your equation for dh/dt: h cannot = qin - qout, you've already written dh/dt = qin - qout (which was incorrect also).

What is the correct relationship between dh/dt and qin - qout? (Hint: area of the bottom of the tank is a factor). And, once you get dh/dt right, how does one go from dh/dt to h?
 
Thanks for pointing that out, so I came to the idea that

a*dh/dt = dv/dt = q_in(t) - q_out(t) = 0 for steady state

which would make the rest of the derivation ok I hope?

Which then gave me a different drawing for the block diagram.

image.jpg


Which gives me a loop gain of (c_1 - c_2)/as

Instead of the c_1 / c_2 i got when I used the assumption that dv/dt = 0 for steady state. Am I still wrong with my equations or drawing?

I thought I had it for a minute there! Thanks for your help. I don't need to do it, it's just bugging me as I cannot relate it to the rest of my notes.
 
Your block diagram is now correct.

Loop gain = H(s)/H0(s).
 
Thanks again mate, I played with it some more, got the answers I wanted and have a much better understanding of signal flow graphs and masons formula.
 

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