Modelling of Electrical systems_newhi.pdf

DuraiRaj315751 7 views 21 slides Sep 27, 2024
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About This Presentation

Modelling of electrical system


Slide Content

Basis Electrical Elements
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Electrical System
•Composed of resistors, capacitors, inductors,
transistors, amplifiers, power supplies
–Passive circuits: respond to applied voltage or current and
do not have any amplifiers
–Active circuits: made of transistors and/or amplifiers,
require active power source to work
•Basic quantities
–Charge q [coulomb] = 6.24x10
18
electrons
–Current i[ampere] = dq/dt
–Voltage e [Volt] = dw/dq
–Energy or Work w [joule]
–Power p [watt] = e x i= dw/dt
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Units and Representations for Common Electrical Quantities
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Equivalent Circuit for Spring-Mass-
Dashpot Systems
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Resistance
•Resistance behavior is between insulator and
conductors, allowing a predictable restriction
of electron flow
•Power dissipated =
•Resistance
–A: cross section are of wire
–l: length of wire
–ρ: resistivity of material
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Capacitance
•Capacitor stores electrons on 2 parallel plates
separated by an insulating dielectric material in an
electric field
•Energy stored in capacitor
•Capacitance
–A: area of plates
–D: spacing between plates
–ϵ:permittivity of the dielectric
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or

Inductance
•Inductance relates voltage induced to time
rate of change of magnetic field
•Faraday’s law:
where φis the magnetic flux, φ = Li
•Energy stored:
•Inductance:
where A= wire cross section area, l = wire length, n =
number of turns, μ
m=permeability of magnetic
circuit
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Impedance
•Impedance Z: instantaneous ratio of voltage
difference to current
•Impedance of common circuit elements
–Resistive: Z
r= R (not dynamic)
–Capacitive: Z
c= 1/CD
–Inductive: Z
L=LD
Where D= differential operator d/dt,
1/D = integrator operator
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Ideal and Non-Ideal Sources
Voltage SourceCurrent Source
Ideal
Non-Ideal
Battery
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Open and Short Circuits
•An open circuit is any element through which
current cannot flow
•A short circuit is any element across which
there is no voltage
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Series and Parallel
Impedance Combinations
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R
L
C

Laws for Passive Circuit Analysis
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Techniques for Passive Circuit Analysis for
Classical Deriving Differential Equations
1.Draw circuit schematic and label components (e.g., R
1, R
2, C
1,
L
1…)
2.Assign voltage at each node (e.g., e
1, e
2)
3.Assign current in each component (e.g., i
1, i
2, ..) and show
positive current direction with arrows
4.Write equation for current for each component (e.g., i
R1=
(e
1-e
2)/R
1or i
C1= CDe
1)
5.Write node equations for each significant node (not
connected to voltage or current source)
6.Substitute component equations into node equations and
reduce results to a single differential equation with output
and input variables
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Example 1: Voltage Divider
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Evaluate e
1

Example 2: Resistor Circuit
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•Calculate the amount of power dissipated in resistor R
3in the
circuit shown below
•Solution:

Example 3: Pair-Share Exercise
Seven-Resistor Circuit
•The resistive circuit shown consists of a voltage source
connected to a combination of seven resistors. The output is
voltage e
0. Find the equivalent resistance R
eqof the seven-
resistor combination and evaluate e
0.
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Example 3: Pair-Share Exercise
Seven-Resistor Circuit
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Apply voltage divider equation repeatedly

Example 4: Dual RC Circuit
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•Write the modeling equations for circuit (a)
•Derive the differential equation in the form [τD+1]e
1=Ge
0
•What are the mathematical expressions for time constant τ
and gain G?
•For circuit (b), is the differential equation for this circuit a
product of two RC’s circuit, that is, [τ
1D+1][τ
2D+1]e
2=e
0?

Example 4: Dual RC Circuit
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(a)
i
R1
i
C1

Example 4: Dual RC Circuit
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(b)
i
R1
i
C1
i
R2
i
C2

Example 4: Dual RC Circuit
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