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Page 1: Dynamic analysis of dc machine

PHYSICAL STRUCTURE9

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PE 9211 Analysis of Electrical Machines

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Dynamic Characteristics of Permanent Magnet DC Motor

Modes of Dynamic operation

1. Starting from stall

2. Changes in load torque

Condition: The machine supplied from a

constant – voltage source

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Mathematical Model of a PMDC Motor: 9

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This motor consists of two first order differential equation and two

algebraic equation

Armature current equation,

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Speed equation,

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Simulink Model of PMDC Motor

Motor Parameters

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Solving armature current equation

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Solving Speed equation

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Dynamic performance during starting

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Dynamic Characteristics of DC Shunt Motor

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Simulink Model of DC Shunt Motor:

Fig shows the Simulink model of DC Shunt Motor. It is constructed using

subsystems for solving each differential equations (i.e.) armature

current, field current and torque equation.

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Time domain block diagrams and state equations

Shunt connected dc machine

W.K.T

𝒗𝒂 = π’Šπ’‚π’“π’‚ + 𝑳𝑨𝑨 π’…π’Šπ’‚π’…π’•

+ π‘³π‘¨π‘­πŽπ’“π’Šπ’‡ βˆ’ βˆ’ βˆ’βˆ’ 𝟏

𝒗𝒇 = π’Šπ’‡π‘Ήπ’‡ + 𝑳𝑭𝑭 π’…π’Šπ’‡

𝒅𝒕 βˆ’ βˆ’ βˆ’βˆ’ 𝟐

𝑻𝒆 = 𝑻𝑳 + 𝑱 π’…πŽπ’“

𝒅𝒕 + π‘©π’ŽπŽπ’“ βˆ’ βˆ’βˆ’ βˆ’ πŸ‘

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Equations (1),(2) and (3) can be written in terms of its time constants

𝒗𝒂 = 𝒓𝒂 𝟏 + 𝑳𝑨𝑨

𝒓𝒂

𝒅

𝒅𝒕 π’Šπ’‚ + π‘³π‘¨π‘­πŽπ’“π’Šπ’‡

𝒗𝒂 = 𝒓𝒂 𝟏 + 𝝉𝒂 𝝆 π’Šπ’‚ + π‘³π‘¨π‘­πŽπ’“π’Šπ’‡βˆ’βˆ’βˆ’βˆ’βˆ’βˆ’ πŸ’

𝑯𝒆𝒓𝒆, 𝝆 βŸΆπ’…

𝒅𝒕

𝒗𝒇 = 𝑹𝒇 𝟏 + 𝑳𝑭𝑭

𝑹𝒇

𝝆 π’Šπ’‡

𝒗𝒇 = 𝑹𝒇 𝟏 + 𝝉𝒇 𝝆 π’Šπ’‡βˆ’βˆ’βˆ’βˆ’βˆ’βˆ’βˆ’(5)

𝑻𝒆 βˆ’ 𝑻𝑳 = ( π‘©π’Ž + 𝑱 𝝆) πŽπ’“ βˆ’βˆ’ βˆ’ βˆ’ πŸ”

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𝝉𝒂 ⟢ Armature time constant

𝝉𝒇 ⟢ Field time constant

π‘Ίπ’π’π’—π’Šπ’π’ˆ 𝒕𝒉𝒆 π’†π’’π’–π’‚π’•π’Šπ’π’π’” πŸ’ , πŸ“ 𝒂𝒏𝒅 πŸ” 𝒇𝒐𝒓 π’Šπ’‚ ,

π’Šπ’‡, 𝒂𝒏𝒅 πŽπ’“ π’šπ’Šπ’†π’π’…π’”

π’Šπ’‚ =

πŸπ’“π’‚

𝝉𝒂𝝆 + 𝟏 𝒗𝒂 βˆ’ π‘³π‘¨π‘­πŽπ’“π’Šπ’‡ βˆ’ βˆ’ βˆ’βˆ’ πŸ•

π’Šπ’‡ =

πŸπ‘Ήπ’‡

𝝉𝒇𝝆 + 𝟏 𝒗𝒇 βˆ’ βˆ’βˆ’ βˆ’ πŸ–

πŽπ’“ =𝟏

𝑱𝝆 + π‘©π’Ž 𝑻𝒆 βˆ’ 𝑻𝑳 βˆ’βˆ’ βˆ’ βˆ’ πŸ—

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Time domain block diagram of a shunt connected dc machine

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π‘Ίπ’π’π’—π’Šπ’π’ˆ 𝒕𝒉𝒆 π’†π’’π’–π’‚π’•π’Šπ’π’π’” 𝟏 , 𝟐 𝒂𝒏𝒅 πŸ‘ 𝒇𝒐𝒓 π’…π’Šπ’‚

𝒅𝒕, π’…π’Šπ’‡

𝒅𝒕

𝒂𝒏𝒅 π’…πŽπ’“

𝒅𝒕 π’šπ’Šπ’†π’π’…π’”

From (1)

π’…π’Šπ’‚π’…π’•

= βˆ’π’“π’‚

𝑳𝑨𝑨

π’Šπ’‚ βˆ’ 𝑳𝑨𝑭

𝑳𝑨𝑨

π’Šπ’‡πŽπ’“ + 𝟏

𝑳𝑨𝑨

𝒗𝒂— 𝟏𝟎

From (2)

π’…π’Šπ’‡

𝒅𝒕= βˆ’

𝑹𝒇

𝑳𝑭𝑭

π’Šπ’‚ + 𝟏

𝑳𝑭𝑭

𝒗𝒇— 𝟏𝟏

From (3)

π’…πŽπ’“

𝒅𝒕= βˆ’

π‘©π’Ž

π‘±πŽπ’“ +

𝑳𝑨𝑭

π‘±π’Šπ’‡π’Šπ’‚ βˆ’

𝟏

𝑱𝑻𝑳 βˆ’ βˆ’(𝟏𝟐)

State equation of shunt dc machine

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𝜌

π’Šπ’‡π’Šπ’‚πŽπ’“

=

βˆ’π‘Ήπ’‡

π‘³π‘­π‘­πŸŽ 𝟎

πŸŽβˆ’π’“π’‚

π‘³π‘¨π‘¨πŸŽ

𝟎 πŸŽβˆ’π‘©π’Ž

𝑱

π’Šπ’‡π’Šπ’‚πŽπ’“

+

πŸŽβˆ’π‘³π‘¨π‘­πŽπ’“

𝑳𝑨𝑨

π‘³π‘¨π‘­π’Šπ’‡π’Šπ’‚

𝑱

+

𝟏

π‘³π‘­π‘­πŸŽ 𝟎

𝟎𝟏

π‘³π‘¨π‘¨πŸŽ

𝟎 πŸŽβˆ’πŸ

𝑱

𝒗𝒇

𝒗𝒂

𝑻𝑳

State equations in matrix form or vector matrix form

Note: The second term on the right side contains the product of state

variables causing the system to be nonlinear.

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Permanent Magnet dc Machine

𝒗𝒇 π’Šπ’” π’†π’π’Šπ’Žπ’Šπ’π’‚π’•π’†π’…

π‘³π‘¨π‘­π’Šπ’‡ π’Šπ’” 𝒓𝒆𝒑𝒍𝒂𝒄𝒆𝒅 π’ƒπ’š π’Œπ’—

π’Œπ’— π’Šπ’” π’…π’†π’•π’†π’“π’Žπ’Šπ’π’†π’… π’ƒπ’š

Strength of the magnetReluctance of the ironNo. of turns in the armature winding

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W.K.T

Above eqns. (1) and (2) can be written in terms of its time constants

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29Time domain block diagram of a permanent magnet DC machine

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State Equation of a permanent magnet DC machine

From (1)

From (2)

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The form in which the state equations are expressed in above eqn.

is called the fundamental form.

OR

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Advantages to using the state space representation compared with other methods.

1.The ability to easily handle systems with multiple inputs and outputs;

2.The system model includes the internal state variables as well as the output variable;

3.The model directly provides a time-domain solution, the matrix/vector modeling is very efficient from a computational standpoint for computer implementation

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404349

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