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MATLAB CHAPTER 9 Simulink

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Title: MATLAB CHAPTER 9 Simulink


1
MATLAB ??CHAPTER 9 Simulink

2
Simulation Diagram
  • Simulation diagram (block diagram)
  • Consider the equation
  • ?
  • ?
  • Simulation diagrams for

3
Introduction to Simulink
  • Type Simulink
  • in the MATLAB
  • Command window
  • to start window.

? The Simulink Library Browser
4
Introduction to Simulink
  • Create a new model
  • Click on the icon that resembles a clean sheet of
    paper, or select New from the File menu in the
    Browser.

Click this icon
Or File ? New
5
Introduction to Simulink
  • ? Double-click appropriate library.
  • ? See a list of blocks within that library.
  • ? Click on the block name or icon.
  • ? Hold the mouse button, and drag
  • it to the new model window.
  • ? release the button.

click, hold, drag, and release
6
Introduction to Simulink
  • ? Use the File menu in the model window to Open,
    Close, and Save model files.
  • ? To print, File ? print
  • ? Edit to copy, cut and paste blocks.
  • ? you can also use mouse for these operations

7
Introduction to Simulink
  • E.g.
  • Simulink Solution of
  • Use Simulink to solve the following problem for
    0 t 13.
  • The exact solution is

8
Introduction to Simulink
  • ? Start Simulink and open a new model window.
  • ? Select and place the Sine Wave block from the
    Source library.
  • Double-click to open the Block Parameters
    window.
  • Make sure Amplitude 1, Frequency 1, Phase
    0, Sample time 0
  • Then click OK.

9
Introduction to Simulink
  • ? Select and place the Gain block from the Math
    Operations library.
  • the Block Parameters window the Gain value
    10.
  • Note that the value 10 then appears in
    the triangle.
  • ? Select and place the Integrator block from the
    Continuous library.
  • Initial condition0 (because y(0)0)

10
Introduction to Simulink
  • ? Select and place the Scope block from the Sinks
    library.
  • ? connect each input and output port.

11
Introduction to Simulink
  • ? click on the Simulation menu, and click the
    Configuration Parameters item.
  • click on the solver tab, and enter 13 for
    the stop time.
  • Make sure the Start time is 0.
  • (matlab 6.5 click Simulation parameters)

matlab 6.5 Simulation parameters
12
Introduction to Simulink
  • ? Run the simulation by clicking on the
    Simulation menu,
  • and clicking the Start item.

13
Introduction to Simulink
  • ? After the simulation, double-click on the Scope
    block .

Double-click!
14
Linear State-Variable Models
  • State-variable models can have more than one
    input and more than on output.
  • Simulink has the State-space block that
    represents the linear state-variable model
  • E.g.
  • Simulink Model of the Two-Mass System

15
Linear State-Variable Models
  • m15, m23, c14, c28, k11, and k24
  • The eq. of motion are
  • These equations can be expressed in
    state-variable form as

16
Linear State-Variable Models
  • Vector matrix form
  • Initinal condition

17
Linear State-Variable Models
  • Solution
  • ?Create a new model window
  • ?Select and place the Step block from the Sources
    library.
  • Step time0, Initial and Final values 0 and
    1, Sample time0

18
Linear State-Variable Models
  • ?Select and place the State-Space lock. Enter
    A,B,C,D. Then enter initial condition.
  • ?Select and place the Scope block.
  • ?connect each port.

19
Linear State-Variable Models
  • ?experiment with different values of the Stop
    time until the Scope shows that the steady-state
    response has been reached.
  • Ex) when stop time 25

steady-state
20
Piecewise-Linear Models
  • Closed-form solutions are not available for most
    nonlinear differential equations, We must solve
    such equations numerically.
  • Ex)
  • Piecewise-linear models are actually nonlinear,
    although they may appear to be linear.
  • Ex) a mass attached to a spring and sliding on a
    horizontal surface with Coulomb friction.

21
Piecewise-Linear Models
  • These two equations can be expressed as the
    single, nonlinear equation.
  • Solutions of models that contain piecewise-linear
    functions are very tedious to program. However,
    Simulink has built-in blocks that represent many
    of the commonly-found functions such as Coulomb
    friction. Therefore Simulink is especially
    useful for such applications. One such block is
    the Saturation block in the Discontinuities
    library.

22
Simulink Model of a Rocket-Propelled sled
  • A rocket propelled sled
  • Compute the sleds velocity v for 0t6 if v(0)
    0
  • The rocket thrust is 4000N and the sled mass is
    450kg.
  • The sleds equation of motion is

23
Simulink Model of a Rocket-Propelled sled
  • To obtain ?(t)
  • Thus the equation of motion becomes
  • The solution is formally given by

24
Simulink Model of a Rocket-Propelled sled
  • (a) Create a Simulink model to solve this problem
    for 0t10s.
  • (b) Now suppose that the engine angle is limited
    by a mechanical stop to 60 , which is 60p/180
    rad. Create a Simulink model to solve the
    problem.
  • Solution
  • (a)
  • ?create ?(t) by integrating the constant
    twice.
  • ?Constant block from the Sources library.
    Constant valuepi/50.
  • ?Trigonometric block from the Math Operations
    library. Functioncos.

25
Simulink Model of a Rocket-Propelled sled
  • ? Set the Stop time 10, run the simulation, and
    examine the result in Scope.
  • (b)
  • ?modify the model as follows.
  • ?the Saturation block from the Discontinuities
    library.
  • Upper limit 60pi/180,
  • Lower limit0.
  • ?mux

mux
Generate the solution when the engine angle ?0.
26
Simulink Model of a Rocket-Propelled sled
  • Scope window

T0
T?0
27
The Relay Block
  • The Simulink Relay block is an example of
    something that is tedious to program in MATLAB
    but is easy to implement in Simulink.
  • A graph of the logic of a relay.
  • The relay switches the output between two
    specified values, named On and Off in the figure.

28
Model of a Relay-Controlled Motor
  • The model of an armature-controlled dc motor

29
Model of a Relay-Controlled Motor
  • x1i, x2?
  • R0.6?, L0.002H, KT0.04Nm/A, Ke0.04Vs/rad,
    c0.01Nms/rad, and I610(-5)kgm2
  • Suppose we have a sensor that measure the motor
    speed, and we use the sensors signal to activate
    a relay to switch the applied voltage v(t)
    between 0 and 100V to keep the speed between 250
    and 350rad/s.
  • SwOff250, SwOn350, Off100, On0

30
Model of a Relay-Controlled Motor
  • Given parameter values
  • To examine the speed ? as output, we choose

31
Model of a Relay-Controlled Motor
  • ?Create a new Simulink model.
  • ?Select and place a Step block from the Sources
    library. Label it Disturbance Step.
  • Step time0.05, Initial and Final time0 and 3,
    Sample time0
  • ?Select and place a Relay block from the
    Discontinuities library.
  • Switch-on and Switch-off points350 and 250,
  • Output when on and Output when off0 and 100.

32
Model of a Relay-Controlled Motor
  • ?Select and place the Mux block from the signal
    Routing library.
  • Display option to Signals.
  • number of input2.
  • ?Select and place the State-Space block from the
    Continuous library.
  • enter the A,B,C,D.
  • enter 00 for the initial conditoin.
  • B tells 2 input, C and D tells 1 output.

33
Model of a Relay-Controlled Motor
  • ?Select and place the Scope block from the Sinks
    library.
  • ?connect each port.
  • ?Stop time0.1 and run the simulation. (the plot
    of ?(t) in the scope.)
  • ?If you want examine the current i(t), change
    the matrix C to 1,0, and run the simulation
    again.

Note Connect signal1(first input) to the output
of the Relay block Connect signa2(second input)
to the output of the Disturbance Step
34
Model of a Relay-Controlled Motor
  • Relay logic scheme keeps the speed within the
    desired limits of 250 and 350 before the
    disturbance torque starts to act.
  • Speed oscillates.
  • When V0, the speed decrease because back emf,
    and viscous damping.
  • The speed drops below 250 when the disturbance
    torque starts to act, because the V0.
  • As soon as the speed drops for the speed to
    increase because the motor torque must now work
    against the disturbance.

35
Model of a Relay-Controlled Motor
  • Speed becomes constant
  • V100, the system achieves a steady-state
    condition in which the motor torque equals the
    sum of the disturbance torque and the viscous
    damping torque. Thus the acceleration is zero.

Change the matrix C1,0 Current i(t)
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