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Three-Phase circuits Prof. Siripong Potisuk
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Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Dec 22, 2015

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Page 1: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Three-Phase circuits

Prof. Siripong Potisuk

Page 2: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Faraday’s Law

“The EMF induced in a circuit is directly proportional to the time rate of change of magnetic flux through the circuit.”

The EMF can be produced by changing B (inducedEMF) or by changing the area, e.g., by moving thewire (motional EMF).

It is the relative movement between the coil and the magnet that matters

Page 3: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

brush

Slip ring

MagneticFlux lines

Magnet

DC source

Conductorloop

Coil

Page 4: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Start ¼ Cycle

½ Cycle ¾ Cycle

¼ C

ycle

½ C

ycle

¾ C

ycle

Page 5: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.
Page 6: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.
Page 7: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

¾ C

ycle

½ C

ycle

¼ C

ycle

Sta

rt

Phase 1

Phase 2

Phase 3

Page 8: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Three-phase Voltage Sources

Y-connected Source -connected Source

Page 9: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced Y-connected Voltage Source

• Balanced phase voltages are equal in magnitude and are out of phase with one another by 120 degrees.

• Phase voltages sum up to zero.• Two possible combinations:

abc or (+) sequence acb or () sequence

Page 10: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced Y-connected Voltage Source

• Balanced line voltages are equal in magnitude and are out of phase with one another by 120 degrees.

• Line voltages sum up to zero.• The magnitude of line voltages is 1.732 times the magnitude of

the phase voltages• Line Voltages lead their corresponding phase voltages by 30

degrees

Page 11: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced Three-phase Load Configurations

Y-connected Load -connected Load

A balanced load is one in which the phase impedances are equalin magnitude and in phase.

Page 12: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced Y-Y Connection

ZY = ZS + Zl + ZL

Page 13: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Example Calculate the line currents in the three-wire Y-Y system as shown.

Page 14: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced Y- Connection

Page 15: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Example A balanced abc-sequence Y-connected source with V is connected to a -connected balanced load of 8+j4 per phase. Calculate the phase and the line currents.

10100anV

Page 16: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced - Connection

Page 17: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Example A balanced -connected load having an impedance of 20-j15 is connected to a -connected, positive sequence generator having 0330abV V. Calculate the phase

currents of the load and the line currents.

Page 18: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Balanced -Y Connection

Page 19: Three-Phase circuits Prof. Siripong Potisuk. Faraday’s Law “The EMF induced in a circuit is directly proportional to the time rate of change of magnetic.

Example A balanced Y-connected load with a phase impedance of 40+j 25 is connected to a balanced, positive sequence -connected source with a line voltage of 210 V. Calculate the phase currents. Use Vab as reference.