Fundamentals Mechanical Power of Power2 Wattmeter Method 3 Wattmeter Method ƒ Time Domain equency...

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Fundamentals of Power Measurement Unit Relationships Average, RMS, Peak, Peak-to-Peak Conversation Known Value Average RMS Peak Peak-to-Peak Average 1.0 1.11 1.57 3.14 RMS 0.9 1.0 1.414 2.828 Peak 0.637 0.707 1.0 2.0 Peak-to-Peak 0.32 0.3535 0.5 1.0 Three Phase System Balanced three phase diagram V line-line = V line-neutral 3 Mechanical Power P m = x Torque 2 x π x Rotating Speed 60 (Sec/Min) Synchronous Speed = 120 x Frequency Number of Poles Electrical Power DC Power Measurement Watts W = V x A AC Power Measurement Active Power Watts P = V rms x A rms x Cosɸ Reactive Power VARS Q = V rms x A rms x Sin ɸ Apparent Power Volt-Amps S = V rms x A rms Efficiency = Output Power Input Power = P m Electrical Input Power ɸ P Q S POWER RELATIONSHIPS VOLT-AMPS VARS WATTS Displacement Power Factor PF = Cosɸ True Power Factor The Precision Makers A WORD OF CAUTION NEVER Open circuit the secondary side of a current transformer while it is energized! This could cause serious damage to the CT and could possibly be harmful to equipment operators. W VA PF = WATTS P = Power VOLTS V = Voltage AMPS I = Current OHMS R = Resistance PxR V x I I x R I 2 x R V 2 R P I P I 2 V 2 P V R P V V I P R Watts P Amps I V Volts R Ohms

Transcript of Fundamentals Mechanical Power of Power2 Wattmeter Method 3 Wattmeter Method ƒ Time Domain equency...

Page 1: Fundamentals Mechanical Power of Power2 Wattmeter Method 3 Wattmeter Method ƒ Time Domain equency Domain time Amplitude or non-sinusoidal waveform consist of Sine Waves of various:

Fundamentalsof Power

Measurement

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����

Unit Relationships

Average, RMS, Peak,Peak-to-Peak Conversation

Known Value Average RMS Peak Peak-to-Peak

Average 1.0 1.11 1.57 3.14

RMS 0.9 1.0 1.414 2.828

Peak 0.637 0.707 1.0 2.0

Peak-to-Peak 0.32 0.3535 0.5 1.0

Three Phase System

Balanced three phase diagram

V line-line = V line-neutral3� ❉

Mechanical Power

Pm = x Torque2 x π x Rotating Speed

60 (Sec/Min)

Synchronous Speed = 120 x FrequencyNumber of Poles

Electrical PowerDC Power Measurement

Watts W = V x A

AC Power Measurement

Active Power

Watts P = Vrms x Arms x Cosɸ

Reactive Power

VARS Q = Vrms x Arms x Sinɸ

Apparent Power

Volt-Amps S = Vrms x Arms

Efficiency = Output PowerInput Power = Pm

ElectricalInput Power

ɸP

QSPOWER RELATIONSHIPS

VOLT-AMPS VARS

WATTS

Blondel TransformationBlondel theory states that total power is measured with

ONE LESS wattmeter than the number of WIRES.

1-P 2-W 1 Wattmeter1-P 3-W 2 Wattmeters3-P 3-W 2 Wattmeters3-P 3-W 3 Wattmeters3-P 4-W 3 Wattmeters

Displacement Power Factor

PF = Cosɸ

True Power Factor

Harmonic Measurements

Ʃ

Ʃ

Ʃ

���

����

����

P = ∫0

T v(t) * i (t) dt

∫0

T v(t)2 dt

∫0

T i(t)2 dt

URMS =

IRMS = I =

U =

P = P (k)

U (k )2

I (k ) 2

max

max

max

k = min

k = min

k = min

k = Harmonic Order; 1, 2, 3, . . .etc

k = Harmonic Order; 1, 2, 3, . . .etc

Harmonics ModeNOT True RMS Measurement

Typical UL and CSA Method

Typical IEC Method

* 100

* 100

ITHD =

ITHD =

max

k = 2

I (k=1)

I (k)2

Normal ModeTrue RMS Measurement

ThePrecisionMakers

Functions WT1800Power Analyzer

DLM2000Oscilloscope

Bandwidth DC - 2MHz DC - 500MHzPower DC - 50MHz

Accuracy 0.05% reading +0.1% range

Calibrated Traceable Measurement System

1.5% at input terminals, at DC

Power approx at 3.5%Based on Probe Accuracy

Input Method Direct Connections to High Voltage & High Current

Probes for high frequency & small currents

Resolution Typical 16-bit 65,636 levels

Typical 8-bit256 levels

PFT =Wa + Wb

(VAa + VAb)

�PFT =

Wa + Wb

33 (VAa + VAb + VAc)

∑���max

k = 2

I ( Total )

I (k)2

ACSource

A

V

V

W

W

+-

+-

+-

V(t)

V(t)

I(t)

One-phaseThree-wire

Load1P-3W

I(t)

A

Phase A

Phase B

Neutral

a

b

ACSource

AW

+-

V

V

Three-phaseThree-wire

Load3P-3W

Phase A

Phase C

Phase B

a

ab

cb

W+-

bA

W+-c

A +-

Vac

+-+-

V

V

V

ACSource

AW

+-

V

V

Three-phaseThree-wire

Load3V-3A

Phase A

Phase C

Phase B

a

ab

cb

W+-

bA

W+-c

A +-

Vac

+-+-

V

V

V

Three-phaseFour-wire

Load3P-4W

Van

Vbn

Vcn

AW

+-c

AW

+-b

AW

+-a

V

V

V

Phase A

Phase C

Phase BAC

Source

+-

ACSource

A

VW

+-

+-

V(t)I(t) One-phase

Two-wireLoad

1P-2W

a

PT = Wa + Wb

PT = Wa + Wb

PT = Wa + Wb

PT = Wa + Wb + Wc

A WORD OF CAUTION

NEVER Open circuit the secondary side of a current transformer while it is energized!

This could cause serious damage to the CT and could possibly be harmful to equipment operators.

Power Analyzer vs Oscilloscope

�PFT =

Wa + Wb

32 (VAa + VAb)

PFT =Wa + Wb + Wc

(VAa + VAb + VAc)

PT = Wa

PFT =Wa

VAa

1 Wattmeter Method

2 Wattmeter Method

3 Wattmeter Method

ƒ

Frequency DomainTime Domain

time

Ampl

itude

Elements of a distortedor non-sinusoidalwaveform consist of Sine Waves of various:� Amplitudes� Frequencies� Phase

Because of the Phasedifference in some ofthe harmonics, negative,or reverse power canactually be produced.

Harmonics are defined as Voltages, Currents or Power at frequencies that are a multiple of the fundamental frequency.Total Power of the Distorted Waveform is calculated as:Ptotal= V0 x I0 + V1 x I1 x Cosθ1 + V2 x I2 x Cosθ2 + V3 x I3 x Cos03 +...+Vn x In x Cosθn

OR More Precisely

Ptotal= V0 x I0 + Ʃmin Vn x In x Cosθn

Distorted AC Waveforms

1T

1T

1T

WVAPF =

Yokogawa Deutschland GmbH | Tel. +49 8152 9310-0 | [email protected] | tmi.yokogawa.com/de

Test&Measurement

WATTSP = Power

VOLTSV = Voltage

AMPSI = Current

OHMSR = Resistance

�PxR

V x I

I x R

I2 x R

V2

—R

P—IP— I2

V2

—P

V— R P—V

V—I

P— RWatts

PAmps

IV

VoltsR

Ohms

Page 2: Fundamentals Mechanical Power of Power2 Wattmeter Method 3 Wattmeter Method ƒ Time Domain equency Domain time Amplitude or non-sinusoidal waveform consist of Sine Waves of various:

Fundamentalsof Power

Measurement

����

����

Unit Relationships

Average, RMS, Peak,Peak-to-Peak Conversation

Known Value Average RMS Peak Peak-to-Peak

Average 1.0 1.11 1.57 3.14

RMS 0.9 1.0 1.414 2.828

Peak 0.637 0.707 1.0 2.0

Peak-to-Peak 0.32 0.3535 0.5 1.0

Three Phase System

Balanced three phase diagram

V line-line = V line-neutral3� ❉

Mechanical Power

Pm = x Torque2 x π x Rotating Speed

60 (Sec/Min)

Synchronous Speed = 120 x FrequencyNumber of Poles

Electrical PowerDC Power Measurement

Watts W = V x A

AC Power Measurement

Active Power

Watts P = Vrms x Arms x Cosɸ

Reactive Power

VARS Q = Vrms x Arms x Sinɸ

Apparent Power

Volt-Amps S = Vrms x Arms

Efficiency = Output PowerInput Power = Pm

ElectricalInput Power

ɸP

QSPOWER RELATIONSHIPS

VOLT-AMPS VARS

WATTS

Blondel TransformationBlondel theory states that total power is measured with

ONE LESS wattmeter than the number of WIRES.

1-P 2-W 1 Wattmeter1-P 3-W 2 Wattmeters3-P 3-W 2 Wattmeters3-P 3-W 3 Wattmeters3-P 4-W 3 Wattmeters

Displacement Power Factor

PF = Cosɸ

True Power Factor

Harmonic Measurements

Ʃ

Ʃ

Ʃ

���

����

����

P = ∫0

T v(t) * i (t) dt

∫0

T v(t)2 dt

∫0

T i(t)2 dt

URMS =

IRMS = I =

U =

P = P (k)

U (k )2

I (k ) 2

max

max

max

k = min

k = min

k = min

k = Harmonic Order; 1, 2, 3, . . .etc

k = Harmonic Order; 1, 2, 3, . . .etc

Harmonics ModeNOT True RMS Measurement

Typical UL and CSA Method

Typical IEC Method

* 100

* 100

ITHD =

ITHD =

max

k = 2

I (k=1)

I (k)2

Normal ModeTrue RMS Measurement

ThePrecisionMakers

Functions WT1800Power Analyzer

DLM2000Oscilloscope

Bandwidth DC - 2MHz DC - 500MHzPower DC - 50MHz

Accuracy 0.05% reading +0.1% range

Calibrated Traceable Measurement System

1.5% at input terminals, at DC

Power approx at 3.5%Based on Probe Accuracy

Input Method Direct Connections to High Voltage & High Current

Probes for high frequency & small currents

Resolution Typical 16-bit 65,636 levels

Typical 8-bit256 levels

PFT =Wa + Wb

(VAa + VAb)

�PFT =

Wa + Wb

33 (VAa + VAb + VAc)

∑���max

k = 2

I ( Total )

I (k)2

ACSource

A

V

V

W

W

+-

+-

+-

V(t)

V(t)

I(t)

One-phaseThree-wire

Load1P-3W

I(t)

A

Phase A

Phase B

Neutral

a

b

ACSource

AW

+-

V

V

Three-phaseThree-wire

Load3P-3W

Phase A

Phase C

Phase B

a

ab

cb

W+-

bA

W+-c

A +-

Vac

+-+-

V

V

V

ACSource

AW

+-

V

V

Three-phaseThree-wire

Load3V-3A

Phase A

Phase C

Phase B

a

ab

cb

W+-

bA

W+-c

A +-

Vac

+-+-

V

V

V

Three-phaseFour-wire

Load3P-4W

Van

Vbn

Vcn

AW

+-c

AW

+-b

AW

+-a

V

V

V

Phase A

Phase C

Phase BAC

Source

+-

ACSource

A

VW

+-

+-

V(t)I(t) One-phase

Two-wireLoad

1P-2W

a

PT = Wa + Wb

PT = Wa + Wb

PT = Wa + Wb

PT = Wa + Wb + Wc

A WORD OF CAUTION

NEVER Open circuit the secondary side of a current transformer while it is energized!

This could cause serious damage to the CT and could possibly be harmful to equipment operators.

Power Analyzer vs Oscilloscope

�PFT =

Wa + Wb

32 (VAa + VAb)

PFT =Wa + Wb + Wc

(VAa + VAb + VAc)

PT = Wa

PFT =Wa

VAa

1 Wattmeter Method

2 Wattmeter Method

3 Wattmeter Method

ƒ

Frequency DomainTime Domain

time

Ampl

itude

Elements of a distortedor non-sinusoidalwaveform consist of Sine Waves of various:� Amplitudes� Frequencies� Phase

Because of the Phasedifference in some ofthe harmonics, negative,or reverse power canactually be produced.

Harmonics are defined as Voltages, Currents or Power at frequencies that are a multiple of the fundamental frequency.Total Power of the Distorted Waveform is calculated as:Ptotal= V0 x I0 + V1 x I1 x Cosθ1 + V2 x I2 x Cosθ2 + V3 x I3 x Cos03 +...+Vn x In x Cosθn

OR More Precisely

Ptotal= V0 x I0 + Ʃmin Vn x In x Cosθn

Distorted AC Waveforms

1T

1T

1T

WVAPF =

Yokogawa Deutschland GmbH | Tel. +49 8152 9310-0 | [email protected] | tmi.yokogawa.com/de

Test&Measurement

WATTSP = Power

VOLTSV = Voltage

AMPSI = Current

OHMSR = Resistance

�PxR

V x I

I x R

I2 x R

V2

—R

P—IP— I2

V2

—P

V— R P—V

V—I

P— RWatts

PAmps

IV

VoltsR

Ohms