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CHAPTER II SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” 1
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CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Mar 14, 2020

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Page 1: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

CHAPTER II

SINUSOIDAL STEADY STATE ANALYSIS

“Alternating Current Circuits (A.C.)”

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Page 2: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Objectives

• To review basic facts about sinusoidal signals.

• To introduce Phasors and convert the time domain

sinusoidal waveform into Phasors.

• To develop the phasor relationships for the basic

circuit elements.

• To solve electric circuits in phasor domain.

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Page 3: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Sinusoids

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A periodic function is one that satisfies v(t) = v(t + nT), for all t and for all integers n.

2T

HzT

f1

f 2

• Only two sinusoidal values with the same frequency can be compared by

their amplitude and phase difference.

• If phase difference is zero, they are in phase; if phase difference is not zero,

they are out of phase.

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Phasor

• Transform a sinusoid to and from the time domain to the phasor domain:

(time domain) (phasor domain)

4

)cos()( tVtv m mVV

• Amplitude and phase difference are two principal concerns in the study

of voltage and current sinusoids.

• Phasor will be defined from the cosine function in all our proceeding

study.

• If a voltage or current expression is in the form of a sine, it will be

changed to a cosine by subtracting from the phase.

Page 5: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Phasor

The differences between v(t) and V:

• v(t) is instantaneous or time-domain representation

V is the frequency or phasor-domain representation.

• v(t) is time dependent, V is not.

• v(t) is always real with no complex term, V is generally

complex.

Note: Phasor analysis applies only when frequency is

constant; when it is applied to two or more sinusoid

signals only if they have the same frequency.

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Page 6: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Sinusoid-Phasor Transformation

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Page 7: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

The Phasor

• A phasor is a complex number that

represents the amplitude and phase

of a sinusoid.

• It can be represented in one of the

following three forms:

7

rz

jrez

)sin(cos jrjyxz a. Rectangular

b. Polar

c. Exponential22 yxr

x

y1tanwhere

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Example:

Transform the following sinusoids to phasors:

i = 6 Cos(50t – 40o) A

v = –4 Sin(30t + 50o) V

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Solution:

a. I A

b. Since –sin(A) = cos(A+90o);

v(t) = 4cos (30t+50o+90o) = 4cos(30t+140o) V

Transform to phasor => V V

406

1404

Page 9: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Circuit Elements in Frequency Domain

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VV

i

I

0 t

RV

icos( )mi I t

cos( )

cos( )

m

m

v Ri RI t

V t

rms rmsV RI

rms m

rms m

V VR

I I

Then:

1. Resistance

IV

O0

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Page 11: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

V, i have the same

frequency,V leads i

by 90o

i

Vπ 2π

0 ωt

2. Inductance

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Relationship between voltage and current

sinmi I t

0cos sin( 90 )m m

div L LI t V t

dt

Page 12: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

rms rmsV LI m mV LI

Reactance XL

sinmi I t 0sin( 90 )mv V t

Sinusoidal response of Inductance

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Effective Value

Page 13: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

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Page 14: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

i

v C

sinmv V t

0

0

sin( 90 )

sin( 90 )

m

m

dvi C C U t

dt

I t

Current leads voltage by 90°

2m m mI CV fCV Vi

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3. Capacitors

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Relationship between voltage and current

Page 15: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

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Page 16: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Summary of voltage-current relationship

Element Time domain Frequency

domain

R

L

C

Riv RIV

dt

diLv LIjV

dt

dvCi

Cj

IV

Page 17: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Example

Page 18: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

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Answer: i(t) = 30 cos(100t + 60o) mA

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It is given that the frequency of sinusoidal source is 50Hz, the peak value is 10V,

capacitor is 25μF, determine the peak value of current. If the frequency is 5000Hz,

then what is the peak value of current now?

i

V C

when f =50Hz

6

1 1127.4

2 2 3.14 50 (25 10 )CX

fC

mAAX

V

C

m 78078.04.127

10Im

When f =5000Hz

6

1 11.274

2 2 3.14 5000 (25 10 )CX

fC

AX

VI

C

mm 8.7

274.1

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The higher frequency is under fixed peak value of voltage, the bigger the peak

value of current flowing through capacitor.

Solution

Example

Page 20: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Phasor Domain Sources

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• Convert time domain elements and sources into phasors

Time Domain Phasor Domain

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The Impedance

Page 22: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Kirchhoff’s Laws in the Frequency Domain

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• Both KVL and KCL are hold in the phasor domain or more

commonly called frequency domain.

• Moreover, the variables to be handled are phasors, which

are complex numbers.

• Series and parallel combinations are the same as in D.C.

circuits analysis.

• All the mathematical operations involved are now in

complex domain.

Page 23: CHAPTER II SINUSOIDAL STEADY STATE ANALYSISeee.guc.edu.eg/Courses/Electronics/ELCT401 Electric... · SINUSOIDAL STEADY STATE ANALYSIS “Alternating Current Circuits (A.C.)” ...

Example

Refer to Figure below, determine v(t) and i(t).

Answers: i(t) = 1.118sin(10t – 26.56o) A; v(t) = 2.236sin(10t + 63.43o) V

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Impedance Combinations

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Determine the input impedance of the circuit in figure below

at ω =10 rad/s.

Answer: Zin = 32.38 – j73.76

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