Average Power-Electrical Circuit Analysis-Lecture Slides, Slides of Electrical Circuit Analysis

This lecture is part of lecture series on Electrical Circuit Analysis course. It was delivered by Prof. Mursleen Sayed at Bengal Engineering and Science University. It includes: Average, Power, Resistive, Load, Inductive, Capacitive, Rms, Value, Current, Voltage, Energy

Typology: Slides

2011/2012

Uploaded on 07/23/2012

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Average Power
Average Power,
For Resistive Load
Average Power,
For Inductive & Capacitive Load
Average Power < Pmax
For large Inductive & Capacitive Loads
Average Power = 0
)cos(
2
IV
Piv
mm
2
IV
Pmm
max
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Download Average Power-Electrical Circuit Analysis-Lecture Slides and more Slides Electrical Circuit Analysis in PDF only on Docsity!

Average Power 

Average Power,

For Resistive Load^ 

Average Power,

For Inductive & Capacitive Load^ 

Average Power < P

max

For large Inductive & Capacitive Loads^ 

Average Power = 0

cos( I 2 V P^

i

v

m m^

I 2

V

P^

m m

max

The RMS Value 

Average Power delivered to a resistor^  

RMS value is the effective value of the sinusoidalvoltage or current^ 

Energy delivered by a sinusoidal source of 100 V

rms

in T

sec is the same as the energy delivered by a 100 V dcsource in T sec.

V^ R 2

dt)

t ( cos

V TR

dt

R

t (

cos V

(^1) T P

(^2) m

T t t

v

2

(^2) m

T t t

v

2

(^2) m

0 0

0 0

^

R

I

V R

P

2 rms

(^2) rms

Complex & Apparent Power 

Complex sum of real and reactive power^ 

S = P + jQ ^

units of complex power are volt-amps (VA) ^

Power factor angle

is

θ

= tan

-1^ (Q/P)

Apparent Power is the magnitude of Complex Power^ 

Apparent power is measured in volt-amps (VA)

2

2

Q

P

S^

Complex & Apparent Power 

Apparent power requirements of a device designedto convert electric energy to a non-electric form ismore important than the average power requirement

Average power represents the useful output of theenergy converting device

Apparent power represents the volt-ampere capacityrequired to supply the average power

Complex & Apparent Power 

The power factor of inductive loads iscorrected by adding a capacitor to the deviceitself or connecting capacitors across the linefeeding the load.

Obviously WAPDA cannot get to the devicesa easily as they can get to the line feedingthe area.

Example ^

An electric load operates at 240 V

rms

^

The load absorbs an average power of 8 kW at alagging power factor of 0.

^

Complex power of the load?

^

Impedance of the load?

^

P = 8 kW

cos

^

P = |S|cos

^

|S| = P/cos

= 8/0.8 = 10 kVA

^

Q = |S|sin

= 10sin(36.87) = 6 kVAR

^

S = 8 + j6 kVA

Power Calculations 

S = P + jQ

V

eff

Ieff

*^

V

m

I^ m

θ

θ sin( I 2 Vj

) θ

θ cos( I 2 V

i v m m i v m

m^

^

θ

θ sin(j ) θ

θ cos( I 2 V

i v

i v

m m^

)

(j

m m

i v

e

I 2

V

 

I

V

i

v

eff eff

I 2

V

i

v

m m

(j

eff eff

i v

e

I

V

 

) (j

eff ) (j

eff

i

v^

e

I

e

V

 

docsity.com

Alternate forms for ComplexPower ^

V

eff

Z

Ieff

^

S =

V

eff

I eff

S = Z

Ieff

I eff

S = |

Ieff

Z = |

Ieff

(R + jX)

S = |

Ieff

R + j|

Ieff

X = P + jQ

^

P = |

Ieff

R = I

m

2 R/

^

Q = |

Ieff

X = I

(^2) m

X/

^

S =

V

eff

( V

eff

/ Z)*= |

V

eff

/Z* = P + jQ

^

P = |

V

eff

/R

^

Q = |

V

eff

/X