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Title: Measurement of active and reactive power of three phase
balanced load by one wattmeter method and two wattmeter
method
Presented By
1) Vishal Bholaji Satone
2) Rohit Purushottam Lichade
3) Suraj devanand Gilorkar
4) Gauri Madhavi
 INTRODUCTION
 Power in a three-phase System can be measured by using
the following methods:
1) Two wattmeter method
2) One wattmeter method
. 3) Three wattmeter method
 General Power:
 In d.c. circuits, Power= Voltage× Current.
 But in a.c. circuits, Power Voltage x Current x p.f.
 where, p.f. is a power factor which depends on the phase
difference between voltage and current.
 Power factor 1 i.e. unity if the circuit is purely resistive.
But if the circuit is inductive the p.f. is less than 1 and
lagging. In capacitive circuit, p.f. is leading.
Concept of Active and Reactive power :
 Active Power:
The instantaneous power drawn by an a.c. circuit is
equal to the product of instantaneous values of voltage and
current.
 This power consumed by load
 Active power = VI cosΦ watts
 Reactive power:
The reactive component of current is equal to I sinΦ. The power
drawn by the circuit due to reactive component of current is called as
reactive power.
Reactive power= VI sinΦ VA
One Wattmeter Method of Measuring Power of Three-
Phase Circuit.
 This method is to be used for balanced loads only, and it is
a modification of two wattmeter method of measuring the
power.
 The wattmeter current coil is connected in one line and
the readings of wattmeter are taken by connecting its
pressure coil alternately across the line voltages.
 In balanced 3-wire, 3-phase load circuit the power in each
phase is equal. Therefore, the total power of the circuit can
be determined by multiplying the power measured in any
one phase by three.
 Total power in balanced load = 3 x Power per Phase
 = 3 x Wattmeter reading
• One wattmeter method
by star connection
Phasor Diagram of one wattmeter method
Two wattmeter method of measuring power of
three phase Circuit
 In a three phase three wire system we require 3 elements.
But if we make the common points of the pressure coils
coincide with one of the lines, then we will require only
n- 1= 2 elements.
 Power consumed by load = V1I1 +V2I 2 +v3 I 3
 Instantaneous power P1 = I1 (V1-V3)
 Instantaneous power P2 =I2 (V2-V3)
• Two wattmeter Star connected load
 Sum of the instantaneous reading= Pi + P₂
= I 1(V1-V3) + I 2 (V2- V3)
= I1V1- I1V3 + I2V2 – I2V3
=V1I1+V2 I2 – V3 (I1+I2)
= V1 I1 +V2 I2+V3 I3
 Therefore, the sum of the two wattmeter reading
is equal to the power consumed by the load.
 This is irrespective of whether the load is
balanced or unbalanced.
• Phasor diagram for Two wattmeter
method
• Two wattmeter Delta connected load
 Instantaneous power P1 = -V3 ( i1 – i3 )
P2 = V2 ( i 2 – i 1)
Some of the instantaneous reading of wattmeter p1 and p2 .
P1 +P 2 = -V3 ( i1- i3 ) + V2 ( i2 – i1)
= - V3 i1 +V3 i3 +V2 i2 – V2 i1
= V2i2 + V3i3 – i1( V2 + V3)
A/c. To Kirchhoff's voltage law , v1+v2+v3=0
V1= -(v2+v3)
Sum of the instantaneous reading of two wattmeter =V1I1+V2I2+V3I3
THANKS YOU 🙏

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Rohit lichde .pptx

  • 1. Title: Measurement of active and reactive power of three phase balanced load by one wattmeter method and two wattmeter method Presented By 1) Vishal Bholaji Satone 2) Rohit Purushottam Lichade 3) Suraj devanand Gilorkar 4) Gauri Madhavi
  • 2.  INTRODUCTION  Power in a three-phase System can be measured by using the following methods: 1) Two wattmeter method 2) One wattmeter method . 3) Three wattmeter method  General Power:  In d.c. circuits, Power= Voltage× Current.  But in a.c. circuits, Power Voltage x Current x p.f.  where, p.f. is a power factor which depends on the phase difference between voltage and current.  Power factor 1 i.e. unity if the circuit is purely resistive. But if the circuit is inductive the p.f. is less than 1 and lagging. In capacitive circuit, p.f. is leading.
  • 3. Concept of Active and Reactive power :  Active Power: The instantaneous power drawn by an a.c. circuit is equal to the product of instantaneous values of voltage and current.  This power consumed by load  Active power = VI cosΦ watts  Reactive power: The reactive component of current is equal to I sinΦ. The power drawn by the circuit due to reactive component of current is called as reactive power. Reactive power= VI sinΦ VA
  • 4. One Wattmeter Method of Measuring Power of Three- Phase Circuit.  This method is to be used for balanced loads only, and it is a modification of two wattmeter method of measuring the power.  The wattmeter current coil is connected in one line and the readings of wattmeter are taken by connecting its pressure coil alternately across the line voltages.  In balanced 3-wire, 3-phase load circuit the power in each phase is equal. Therefore, the total power of the circuit can be determined by multiplying the power measured in any one phase by three.  Total power in balanced load = 3 x Power per Phase  = 3 x Wattmeter reading
  • 5. • One wattmeter method by star connection
  • 6.
  • 7. Phasor Diagram of one wattmeter method
  • 8. Two wattmeter method of measuring power of three phase Circuit  In a three phase three wire system we require 3 elements. But if we make the common points of the pressure coils coincide with one of the lines, then we will require only n- 1= 2 elements.  Power consumed by load = V1I1 +V2I 2 +v3 I 3  Instantaneous power P1 = I1 (V1-V3)  Instantaneous power P2 =I2 (V2-V3)
  • 9. • Two wattmeter Star connected load
  • 10.  Sum of the instantaneous reading= Pi + P₂ = I 1(V1-V3) + I 2 (V2- V3) = I1V1- I1V3 + I2V2 – I2V3 =V1I1+V2 I2 – V3 (I1+I2) = V1 I1 +V2 I2+V3 I3  Therefore, the sum of the two wattmeter reading is equal to the power consumed by the load.  This is irrespective of whether the load is balanced or unbalanced.
  • 11. • Phasor diagram for Two wattmeter method
  • 12. • Two wattmeter Delta connected load
  • 13.  Instantaneous power P1 = -V3 ( i1 – i3 ) P2 = V2 ( i 2 – i 1) Some of the instantaneous reading of wattmeter p1 and p2 . P1 +P 2 = -V3 ( i1- i3 ) + V2 ( i2 – i1) = - V3 i1 +V3 i3 +V2 i2 – V2 i1 = V2i2 + V3i3 – i1( V2 + V3) A/c. To Kirchhoff's voltage law , v1+v2+v3=0 V1= -(v2+v3) Sum of the instantaneous reading of two wattmeter =V1I1+V2I2+V3I3