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Mathematical Models of Systems Objectives
We use quantitative mathematical models of physical systems to design and analyze control systems. The dynamic behavior is generally described by ordinary differential equations. We will consider a wide range of systems, including mechanical, hydraulic, and electrical. Since most physical systems are nonlinear, we will discuss linearization approximations, which allow us to use Laplace transform methods. We will then proceed to obtain the input–output relationship for components and subsystems in the form of transfer functions. The transfer function blocks can be organized into block diagrams or signal-flow graphs to graphically depict the interconnections. Block diagrams (and signal-flow graphs) are very convenient and natural tools for designing and analyzing complicated control systems
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Six Step Approach to Dynamic System Problems
Introduction Six Step Approach to Dynamic System Problems Define the system and its components Formulate the mathematical model and list the necessary assumptions Write the differential equations describing the model Solve the equations for the desired output variables Examine the solutions and the assumptions If necessary, reanalyze or redesign the system
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Differential Equation of Physical Systems
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Differential Equation of Physical Systems
Electrical Inductance Describing Equation Energy or Power Translational Spring Rotational Spring Fluid Inertia
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Differential Equation of Physical Systems
Electrical Capacitance Translational Mass Rotational Mass Fluid Capacitance Thermal Capacitance
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Differential Equation of Physical Systems
Electrical Resistance Translational Damper Rotational Damper Fluid Resistance Thermal Resistance
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Differential Equation of Physical Systems
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Differential Equation of Physical Systems
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Differential Equation of Physical Systems
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Differential Equation of Physical Systems
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Linear Approximations
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Linear Approximations
Linear Systems - Necessary condition Principle of Superposition Property of Homogeneity Taylor Series
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Linear Approximations – Example 2.1
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The Laplace Transform Historical Perspective - Heaviside’s Operators
Origin of Operational Calculus (1887)
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Historical Perspective - Heaviside’s Operators
Origin of Operational Calculus (1887) v = H(t) Expanded in a power series (*) Oliver Heaviside: Sage in Solitude, Paul J. Nahin, IEEE Press 1987.
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The Laplace Transform
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The Laplace Transform
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The Laplace Transform
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The Laplace Transform
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The Laplace Transform The Partial-Fraction Expansion (or Heaviside expansion theorem) Suppose that The partial fraction expansion indicates that F(s) consists of a sum of terms, each of which is a factor of the denominator. The values of K1 and K2 are determined by combining the individual fractions by means of the lowest common denominator and comparing the resultant numerator coefficients with those of the coefficients of the numerator before separation in different terms. F s ( ) z1 + p1 p2 × or K1 K2 Evaluation of Ki in the manner just described requires the simultaneous solution of n equations. An alternative method is to multiply both sides of the equation by (s + pi) then setting s= - pi, the right-hand side is zero except for Ki so that Ki pi s = - pi
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The Laplace Transform
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The Laplace Transform Useful Transform Pairs
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The Laplace Transform Consider the mass-spring-damper system
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The Laplace Transform
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
Example 2.2
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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The Transfer Function of Linear Systems
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Block Diagram Models
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Block Diagram Models
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Block Diagram Models Original Diagram Equivalent Diagram
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Block Diagram Models Original Diagram Equivalent Diagram
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Block Diagram Models Original Diagram Equivalent Diagram
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Block Diagram Models
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Block Diagram Models Example 2.7
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Example 2.7 Block Diagram Models
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Signal-Flow Graph Models
For complex systems, the block diagram method can become difficult to complete. By using the signal-flow graph model, the reduction procedure (used in the block diagram method) is not necessary to determine the relationship between system variables.
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Signal-Flow Graph Models
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Signal-Flow Graph Models
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Signal-Flow Graph Models
Example 2.8
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Signal-Flow Graph Models
Example 2.10
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Signal-Flow Graph Models
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Design Examples
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Design Examples Speed control of an electric traction motor.
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Design Examples
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Design Examples
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Design Examples
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Design Examples
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
error Sys1 = sysh2 / sysg4
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
error Num4=[0.1];
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The Simulation of Systems Using MATLAB
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The Simulation of Systems Using MATLAB
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Sequential Design Example: Disk Drive Read System
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Sequential Design Example: Disk Drive Read System
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Sequential Design Example: Disk Drive Read System
=
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P2.11
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P2.11 +Vd Vq Id Tm K1 K2 Km Vc -Vb K3 Ic
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