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Chapter 2

Mathematical Models of

Systems

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Illustrations

2 - 2

Dr. Soleimani, Department of Mechanical Engineering, IAUN

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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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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𝑓 𝑡 𝑑𝑡𝑡

0

𝑒−𝑎𝑡𝑓 𝑡 𝐹(𝑠 + 𝑎)

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

s -> 0 t -> infinite

Lim s F s( ( )) Lim f t( ( ))

7. Final-value Theorem

s -> infinite t -> 0

Lim s F s( ( )) Lim f t( ( )) f 0( )

6. Initial-value Theorem

0

s F s( )

d

f t( ) t 5. Frequency Integration

F s( a) f t( ) e (a t )

4. Frequency shifting

s F s( ) d

d

t f t ( )

3. Frequency differentiation f at( ) 2. Time scaling

1 a F s

 a

 

f t( T) u t ( T)

1. Time delay

e (s T )F s( )

Property Time Domain Frequency Domain

s -> 0 t -> infinite

Lim s F s( ( )) Lim f t( ( ))

7. Final-value Theorem

s -> infinite t -> 0

Lim s F s( ( )) Lim f t( ( )) f 0( )

6. Initial-value Theorem

0

s F s( )

d

f t( ) t 5. Frequency Integration

F s( a) f t( ) e (a t )

4. Frequency shifting

s F s( ) d

d

t f t ( )

3. Frequency differentiation f at( ) 2. Time scaling

1 a F s

 a

 

f t( T) u t ( T)

1. Time delay

e (s T )F s( )

Property Time Domain Frequency Domain

s -> 0 t -> infinite

Lim s F s( ( )) Lim f t( ( ))

7. Final-value Theorem

s -> infinite t -> 0

Lim s F s( ( )) Lim f t( ( )) f 0( )

6. Initial-value Theorem

0

s F s( )

d

f t( ) t 5. Frequency Integration

F s( a) f t( ) e (a t )

4. Frequency shifting

s F s( ) d

d

t f t ( )

3. Frequency differentiation f at( ) 2. Time scaling

1 a F s

 a

 

f t( T) u t ( T)

1. Time delay

e (s T )F s( )

Property Time Domain Frequency Domain

s -> 0 t -> infinite

Lim s F s( ( )) Lim f t( ( ))

7. Final-value Theorem

s -> infinite t -> 0

Lim s F s( ( )) Lim f t( ( )) f 0( )

6. Initial-value Theorem

0

s F s( )

d

f t( ) t 5. Frequency Integration

F s( a) f t( ) e (a t )

4. Frequency shifting

s F s( ) d

d

t f t ( )

3. Frequency differentiation f at( ) 2. Time scaling

1 a F s

 a

 

f t( T) u t ( T)

1. Time delay

e (s T )F s( )

Property Time Domain Frequency Domain

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Differential operator

Integral operator

Final value theorem lim

𝑡→∞

𝑦 𝑡 = lim

𝑠→0

𝑠𝑌(𝑠)

lim

𝑡→0

𝑦 𝑡 = lim

𝑠→∞

𝑠𝑌(𝑠)

Initial value theorem

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Differential Equation:

Laplace Transform:

Transfer Function:

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Rearranged Equations:

Matrix Form:

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Solving for V

1

(s):

Transfer Function:

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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The flux ϕ is proportional to the field current i

f

:

The motor torque is related linearly to ϕ and armature current i

a

:

The field current is related to the field voltage as:

The motor torque T

m

is divided to the load torque T

L

and the

A. Field Control (i

a

=constant)

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

The load torque T

L

for rotating inertia :

Rearranging Equations

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The transfer function of the motor-load combination

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

B. Armature control (i

f

=constant)

The relation between voltage and current of armature:

The motor torque is related linearly to armature current i

a

:

Back electromotive-force voltage:

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Armature current:

Load torque:

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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V2( )s V1( )s

1 RCs

V2( )s

V1( )s RCs

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

( )s Vf( )s

Km

s J s( b)

Lfs Rf

( )s Va( )s

Km

s

Ra Las

(J s b) KbKm
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xo( )t y t( ) xin( )t Xo( )s

Xin( )s

s2

s2 b

M

s

k

M

For low frequency oscillations, where  n Xo j

Xin j

2 k M

V2( )s V1( )s

R2 R

R2 R1 R2

R2

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Gear Ratio = n = N1/N2 N2L N1m

L nm

L nm

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T s( ) q s( )

1 Cts Q S 1

R

 

T To Te = temperature difference due to thermal process Ct = thermal capacitance

= fluid flow rate = constant Q

Y s( ) X s( )

K s Ms( B) K A k x

kp B b A2

kp

kx x d g d

kp P d g d g g x P( ) flow

A = area of piston

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Block diagram of a DC motor

General block representation of two-input, two output system

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Block diagram of interconnected system

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Multi input, multi output system (Matrix form)

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Block Diagram Transformations

Original Diagram Equivalent Diagram

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Block Diagram Transformations

Original Diagram Equivalent Diagram

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Block Diagram Transformations

Original Diagram Equivalent Diagram

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Closed-loop transfer function

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Solution:

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Signal-flow graph of the DC motor

Signal-flow graph of interconnected system

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

Signal-flow graph of two algebraic equation

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

𝑃

𝑘

= یجوزخ هب یدورو سا مُا 𝑘 زیسم هزهب

Δ = فازگ نانیمزتد

Δ

𝑘

= مُا 𝑘 زیسم فذح اب فازگ نانیمزتد

Δ = 1 – ( توافتم یاه هقلح همه هزهب عومجم )

+ ( یسامتزیغ یاه هقلح تفج همه هزهب یزضلصاح عومجم )

– ( یسامتزیغ یاه هقلح هس همه هزهب بزضلصاح عومجم )

+ . . .

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Illustrations

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Dr. Soleimani, Department of Mechanical Engineering, IAUN

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Referensi

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