RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors...

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Revision Lecture 2: Phasors Revision Lecture 2: Phasors Basic Concepts Reactive Components Phasors Phasor Diagram Complex Power Complex Power in Components E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 1 / 7

Transcript of RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors...

Page 1: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Revision Lecture 2: Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 1 / 7

Page 2: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Basic Concepts

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 2 / 7

• Phasors and Complex impedances are only relevant to sinusoidalsources.

A DC source is a special case of a cosine wave with ω = 0.

Page 3: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Basic Concepts

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 2 / 7

• Phasors and Complex impedances are only relevant to sinusoidalsources.

A DC source is a special case of a cosine wave with ω = 0.

• For two sine waves, the leading one reaches its peak first, the laggingone reaches its peak second. So sinωt lags cosωt.

Page 4: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Basic Concepts

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 2 / 7

• Phasors and Complex impedances are only relevant to sinusoidalsources.

A DC source is a special case of a cosine wave with ω = 0.

• For two sine waves, the leading one reaches its peak first, the laggingone reaches its peak second. So sinωt lags cosωt.

• If A cos (ωt+ θ) = F cosωt−G sinωt, then

A =√F 2 +G2, θ = tan−1 G

F.

Page 5: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Basic Concepts

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 2 / 7

• Phasors and Complex impedances are only relevant to sinusoidalsources.

A DC source is a special case of a cosine wave with ω = 0.

• For two sine waves, the leading one reaches its peak first, the laggingone reaches its peak second. So sinωt lags cosωt.

• If A cos (ωt+ θ) = F cosωt−G sinωt, then

A =√F 2 +G2, θ = tan−1 G

F.

F = A cos θ, G = A sin θ.

Page 6: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Basic Concepts

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 2 / 7

• Phasors and Complex impedances are only relevant to sinusoidalsources.

A DC source is a special case of a cosine wave with ω = 0.

• For two sine waves, the leading one reaches its peak first, the laggingone reaches its peak second. So sinωt lags cosωt.

• If A cos (ωt+ θ) = F cosωt−G sinωt, then

A =√F 2 +G2, θ = tan−1 G

F.

F = A cos θ, G = A sin θ.

In CMPLX mode, Casio fx-991ES can do complex arithmetic andcan switch between the two forms with SHIFT,CMPLX,3 orSHIFT,CMPLX,4

Page 7: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Reactive Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 3 / 7

• Impedances: R, jωL, 1

jωC= −j

ωC.

Admittances: 1

R, 1

jωL= −j

ωL, jωC

Page 8: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Reactive Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 3 / 7

• Impedances: R, jωL, 1

jωC= −j

ωC.

Admittances: 1

R, 1

jωL= −j

ωL, jωC

• In a capacitor or inductor, the Current and Voltage are 90 apart :

CIVIL: Capacitor - current leads voltage; Inductor - current lagsvoltage

Page 9: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Reactive Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 3 / 7

• Impedances: R, jωL, 1

jωC= −j

ωC.

Admittances: 1

R, 1

jωL= −j

ωL, jωC

• In a capacitor or inductor, the Current and Voltage are 90 apart :

CIVIL: Capacitor - current leads voltage; Inductor - current lagsvoltage

• Average current (or DC current) through a capacitor is always zero

• Average voltage across an inductor is always zero

Page 10: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Reactive Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 3 / 7

• Impedances: R, jωL, 1

jωC= −j

ωC.

Admittances: 1

R, 1

jωL= −j

ωL, jωC

• In a capacitor or inductor, the Current and Voltage are 90 apart :

CIVIL: Capacitor - current leads voltage; Inductor - current lagsvoltage

• Average current (or DC current) through a capacitor is always zero

• Average voltage across an inductor is always zero

• Average power absorbed by a capacitor or inductor is always zero

Page 11: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 4 / 7

A phasor represents a time-varying sinusoidal waveform by a fixed complexnumber.

Waveform Phasor

x(t) = F cosωt−G sinωt X = F + jG

Page 12: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 4 / 7

A phasor represents a time-varying sinusoidal waveform by a fixed complexnumber.

Waveform Phasor

x(t) = F cosωt−G sinωt X = F + jG [Note minus sign]

Page 13: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 4 / 7

A phasor represents a time-varying sinusoidal waveform by a fixed complexnumber.

Waveform Phasor

x(t) = F cosωt−G sinωt X = F + jG [Note minus sign]

x(t) = A cos (ωt+ θ) X = Aejθ = A∠θ

Page 14: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 4 / 7

A phasor represents a time-varying sinusoidal waveform by a fixed complexnumber.

Waveform Phasor

x(t) = F cosωt−G sinωt X = F + jG [Note minus sign]

x(t) = A cos (ωt+ θ) X = Aejθ = A∠θ

max (x(t)) = A |X| = A

Page 15: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasors

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 4 / 7

A phasor represents a time-varying sinusoidal waveform by a fixed complexnumber.

Waveform Phasor

x(t) = F cosωt−G sinωt X = F + jG [Note minus sign]

x(t) = A cos (ωt+ θ) X = Aejθ = A∠θ

max (x(t)) = A |X| = A

x(t) is the projection of a rotating rod ontothe real (horizontal) axis.

X = F + jG is its starting position at t = 0.

Page 16: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

Page 17: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

Page 18: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

Page 19: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

Page 20: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Page 21: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

Page 22: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

= 0.1− 0.3j = 0.32∠− 72

Page 23: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

= 0.1− 0.3j = 0.32∠− 72

0 0.5 1

-0.4

-0.2

0

Real

Page 24: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

= 0.1− 0.3j = 0.32∠− 72

y(t) = 0.1 cos 300t+ 0.3 sin 300t

0 0.5 1

-0.4

-0.2

0

Real

Page 25: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

= 0.1− 0.3j = 0.32∠− 72

y(t) = 0.1 cos 300t+ 0.3 sin 300t

= 0.32 cos (300t− 1.25)

= 0.32 cos (300 (t− 4.2ms))

0 0.5 1

-0.4

-0.2

0

Real

Page 26: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Phasor Diagram

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 5 / 7

Draw phasors as vectors. Join vectors end-to-end to show how voltages inseries add up (or currents in parallel).

Find y(t) if x(t) = cos 300t .

YX

=1

jωC

R+ 1

jωC

= 1

jωRC+1

= 1

1+3j

= 0.1− 0.3j = 0.32∠− 72

x(t) = cos 300t⇒ X = 1

Y = X × YX

= 0.1− 0.3j = 0.32∠− 72

y(t) = 0.1 cos 300t+ 0.3 sin 300t

= 0.32 cos (300t− 1.25)

= 0.32 cos (300 (t− 4.2ms))

0 0.5 1

-0.4

-0.2

0

Real

0 20 40 60 80 100 120-1

-0.5

0

0.5

1x

y

time (ms)

x=bl

ue, y

=re

d

w = 300 rad/s, Gain = 0.32, Phase = -72°

Page 27: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Page 28: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Page 29: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Page 30: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Apparent Power |S| =∣∣∣V

∣∣∣×∣∣∣I∣∣∣

Page 31: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Apparent Power |S| =∣∣∣V

∣∣∣×∣∣∣I∣∣∣

Average Power P = ℜ (S) = |S| cosφ unit = Watts → heat

Page 32: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Apparent Power |S| =∣∣∣V

∣∣∣×∣∣∣I∣∣∣ unit = VAs

Average Power P = ℜ (S) = |S| cosφ unit = Watts → heatReactive Power Q = ℑ (S) = |S| sinφ unit = VARs

Page 33: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Apparent Power |S| =∣∣∣V

∣∣∣×∣∣∣I∣∣∣ unit = VAs

Average Power P = ℜ (S) = |S| cosφ unit = Watts → heatReactive Power Q = ℑ (S) = |S| sinφ unit = VARs

Conservation of power (Tellegen’s theorem): in any circuit the total complexpower absorbed by all components sums to zero⇒ P = average power and Q = reactive power sum separately to zero.

Page 34: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 6 / 7

If V = |V |∠θV is a phasor, we define V = 1√2× V to be the

corresponding r.m.s. phasor. The r.m.s. voltage is∣∣∣V

∣∣∣ = 1√2× |V |.

Power Factor cosφ = cos (θV − θI)

Complex Power S = V × I∗ = P + jQ [∗ = complex conjugate]

Apparent Power |S| =∣∣∣V

∣∣∣×∣∣∣I∣∣∣ unit = VAs

Average Power P = ℜ (S) = |S| cosφ unit = Watts → heatReactive Power Q = ℑ (S) = |S| sinφ unit = VARs

Conservation of power (Tellegen’s theorem): in any circuit the total complexpower absorbed by all components sums to zero⇒ P = average power and Q = reactive power sum separately to zero.

VARs are generated by capacitors and absorbed by inductors.

φ > 0 for inductive impedance.φ < 0 for capacitive impedance.

Page 35: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z

Page 36: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Page 37: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Page 38: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

Page 39: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

Page 40: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

Page 41: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVA

Page 42: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Page 43: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Add parallel capacitor: 300µF

Page 44: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Add parallel capacitor: 300µFI = 46− 11j = 47∠− 14

Page 45: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Add parallel capacitor: 300µFI = 46− 11j = 47∠− 14

S = V I∗ = 10.9∠14 kVA

Page 46: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Add parallel capacitor: 300µFI = 46− 11j = 47∠− 14

S = V I∗ = 10.9∠14 kVAcosφ = P

|S| = cos 14 = 0.97

Page 47: RevisionLecture2: Phasors - Imperial College London · Phasor Diagram RevisionLecture2: Phasors •Basic Concepts •Reactive Components •Phasors •Phasor Diagram •Complex Power

Complex Power in Components

RevisionLecture 2: Phasors

• Basic Concepts

• Reactive Components

• Phasors

• Phasor Diagram

• Complex Power

• Complex Power inComponents

E1.1 Analysis of Circuits (2014-4472) Revision Lecture 2 – 7 / 7

S = V I∗ =|V |2Z∗

=∣∣∣I∣∣∣2

Z ⇒ ∠S = ∠Z

Resistor: positive real (absorbs watts)Inductor: positive imaginary (absorbs VARs)Capacitor: negative imaginary (generates VARs)

Power Factor Correction

V = 230. Motor is 5||7j Ω.

I = 46− 33j = 56.5∠− 36

S = V I∗ = 13∠36 kVAcosφ = P

|S|= cos 36 = 0.81

Add parallel capacitor: 300µFI = 46− 11j = 47∠− 14

S = V I∗ = 10.9∠14 kVAcosφ = P

|S| = cos 14 = 0.97

Current decreases by factor of 0.810.97

. Lower power transmission losses.