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Lecture slides that review models of electrical circuits and mechanical systems, including differential equations, Laplace Transform, transfer functions, interconnections, and system responses. Learn about R-L-C circuits, Newton's second law, moment of inertia, and more.
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Lecture #9Control EngineeringREVIEW SLIDESReference: Textbook by Phillips and Habor
Models of Electrical Systems • R-L-C series circuit, impulse voltage source:
Kirchhoff’ s voltage law: The algebraic sum of voltages around any closed loop in an electrical circuit is zero. • Kirchhoff’ s current law: The algebraic sum of currents into any junction in an electrical circuit is zero.
Models of Mechanical Systems Mechanical translational systems. • Newton’s second law: • Device with friction (shock absorber): B is damping coefficient. • Translational system to be defined is a spring (Hooke’s law): K is spring coefficient
Model of a mass-spring-damper system: • Note that linear physical systems are modeled by linear differential equations for which linear components can be added together. See example of a mass-spring-damper system.
Mechanical rotational systems. • Moment of inertia: • Viscous friction: • Torsion:
Model of a torsional pendulum (pendulum in clocks inside glass dome); Moment of inertia of pendulum bob denoted by J Friction between the bob and air by B Elastance of the brass suspension strip by K
Differential equations as mathematical models of physical systems: similarity between mathematical models of electrical circuits and models of simple mechanical systems (see model of an RCL circuit and model of the mass-spring-damper system).
Find the inverse Laplace transform ofF(s)=5/(s2+3s+2). Solution:
Find the inverse Laplace transform of F(s)=(2s+3)/(s3+2s2+s). • Solution:
Transfer Function • After Laplace transform we have X(s)=G(s)F(s) • We call G(s) the transfer function.
System interconnections • Series interconnection Y(s)=H(s)U(s) where H(s)=H1(s)H2(s). • Parallel interconnection Y(s)=H(s)U(s) where H(s)=H1(s)+H2(s).
Mason’s Gain Formula • This gives a procedure that allows us to find the transfer function, by inspection of either a block diagram or a signal flow graph. • Source Node: signals flow away from the node. • Sink node: signals flow only toward the node. • Path: continuous connection of branches from one node to another with all arrows in the same direction.
Loop: a closed path in which no node is encountered more than once. Source node cannot be part of a loop. • Path gain: product of the transfer functions of all branches that form the loop. • Loop gain: products of the transfer functions of all branches that form the loop. • Nontouching: two loops are non-touching if these loops have no nodes in common.
An Example • Loop 1 (-G2H1) and loop 2 (-G4H2) are not touching. • Two forward paths:
System Responses (Time Domain) • First order systems: Transient response Steady state response Step response Ramp response Impulse response • Second order systems Transient response Steady state response Step response Ramp response Impulse response
Time Responses of first order systems The T.F. for first order system:
is called the time constant • Ex. Position control of the pen of a plotter fora digital computer: is too slow, is faster.
System DC Gain • In general: