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Circuits II EE221 Unit 12 Instructor: Kevin D. Donohue

Circuits II EE221 Unit 12 Instructor: Kevin D. Donohue. Three Phase Circuits, Balanced Y-Y, Y- , and  -  Three-Phase Circuits. Polyphase Circuits.

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Circuits II EE221 Unit 12 Instructor: Kevin D. Donohue

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  1. Circuits IIEE221Unit 12Instructor: Kevin D. Donohue Three Phase Circuits, Balanced Y-Y, Y-, and - Three-Phase Circuits

  2. Polyphase Circuits Polyphase circuits contain multiple sources at the same frequency but different phases. Power is distributed over the power grid in the form of three-phase sinusoids. Advantages of Three-Phase power distribution include: • (Constant Power) Instantaneous power can be constant in a three phase system. • (More Economical) For equivalent power, the 3-Phase systems are more economical than single-phase (can be driven with lower currents and voltages, and fewer wires required because of a common neutral connection between the phases). • (Flexible) Single phase service can be extracted from the 3-phase systems or phases manipulated to create additional phases.

  3. Balanced 3-Phase Voltages Balanced phase voltage are equal in magnitude and separate by 120 degrees in phase. Voltages generated from a 3-phase generator can have 2 phase sequence possibilities depending on direction of the rotor: Positive sequence (Counter Clockwise Rotation): Negative sequence (Clockwise Rotation): Show that the sum of all phase voltages in a balanced system is zero.

  4. Single and 3-Phase Circuit Comparison Consider the phase voltages of equal amplitude Show that the line voltages are given by: In general: 0º

  5. Balanced 3-Phase Voltage Connections There are 2 ways to connect a Balanced set of sources: Y (wye)-Connected  (delta)-Connected

  6. Balanced Loads Balanced loads are equal in magnitude and phase. There 2 ways to connect balanced loads Y (wye)-Connected  (delta)-Connected Show that for equivalent loads Z = 3ZY A B N C A B C

  7. Load-Source Connections There are 4 possible ways balanced sources and loads can be connected: • Y Source to Y Load (Y-Y) •  Source to  Load (-) • Y Source to  Load (Y-) •  Source to Y Load (-Y) If not specified, the voltages on the sources will be assumed to be in RMS values.

  8. Balanced Y-Y Connection The complete Y-Y connection is shown below with impedances listed separately for the source (subscript s), line (subscript l), and load (subscript L). For a positive sequence with , it can be shown that

  9. Balanced Y-Y Connection Show that the current in each phase can be expressed as: , and that Because of the symmetry of a balanced 3 phase system, the neutral connection can be dropped and the system analyzed on a per phase basis. In a Y-Y connected system, the phase (source or load) and line currents are the same.

  10. Balanced Y- Connection In this case the line voltages are directly across each load. It can be shown that: and the load currents and phase currents are related by: Note the –connected load can be converted to a Y-connected load through:

  11. Balanced  - Connection In this case the line voltages are the phase voltages and are directly across each load. It can be shown that: The line currents can be obtained from the phase currents

  12. Balanced  -Y Connection In this case the phase voltages are across the lines. It can be shown that: the line current is related to the phase voltage by: Note the –connected source can be converted to a Y-connected source through:

  13. Power in Balanced System Show that the instantaneous power absorbed by a load in a balanced Y-Y system is a constant given by: where the impedance in a single phase is given by: The complex power per phase is Note that average power or real power is the same as the instantaneous power for the 3-phase system.

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