Three-phase

Three phase systems have 3 waveforms (usually carrying power) that are 2/3π radians (120 degrees,1/3 of a cycle) offset in time. The figure shows one cycle of a three-phase system, labelled 0 to 360 degrees ( 2 π radians) along the time axis. The plotted line represents the variation of instantaneous voltage (or current) with respect to time. This cycle will repeat 50 or 60 times per second depending on the power system frequency. The colours of the lines represent the American color code for three phase. That is black=VL1 red=VL2 blue=VL3. This article deals with the basic mathematics and principles of three phase. For information on where, how and why Three phase is used please see three-phase electric power. For information on testing three phase kit please see three-phase testing. In this article angles will be measured in radians except where otherwise stated.

variable setup and basic definitions

let x=2\pi ft\,\! where t is time and f is freqency using x the waveforms for the three phases are V_{L1}=A\sin x\,\! V_{L2}=A\sin (x-\frac{2}{3} \pi) V_{L3}=A\sin (x-\frac{4}{3} \pi) where A is the peak voltage and the voltages on L1 L2 and L3 are measured relative to the neutral.

Balanced loads

Generally, in electric power systems the load is distributed as evenly as practical between the phases. It is usual practice to discuss a balanced system first and then describe the effects of unbalanced systems as deviations from the elementary case. To keep the calculations simple we shall normalise A and R to 1 for the remainder of these calculations

star connected systems with neutral

constant power transfer

using R=1 P_{L1}=\frac{V_{L1}^{2}}{R}=V_{L1}^{2}\,\! P_{L2}=\frac{V_{L2}^{2}}{R}=V_{L2}^{2}\,\! P_{L3}=\frac{V_{L3}^{2}}{R}=V_{L3}^{2}\,\! P_{TOT}=P_{L1}+P_{L2}+P_{L3}\,\! P_{TOT}=\sin^{2} x+\sin^{2} (x-\frac{2}{3} \pi)+\sin^{2} (x-\frac{4}{3} \pi) using angle subtraction formulae P_{TOT}=\sin^{2} x+(\sin x\cos(\frac{2}{3} \pi)-\cos x\sin(\frac{2}{3} \pi))^{2}+(\sin x\cos(\frac{4}{3} \pi)-\cos x\sin(\frac{4}{3} \pi))^{2} P_{TOT}=\sin^{2} x+(-\frac{1}{2}\sin x-\frac{\sqrt{3}}{2}\cos x)^{2}+(-\frac{1}{2}\sin x+\frac{\sqrt{3}}{2}\cos x)^{2} P_{TOT}=\sin^{2} x+\frac{1}{4}\sin^{2} x+\frac{\sqrt{3}}{2}\sin x\cos x +\frac{3}{4}cos^{2} x+\frac{1}{4}\sin^{2} x-\frac{\sqrt{3}}{2}\sin x\cos x +\frac{3}{4}cos^{2} x P_{TOT}=\frac{6}{4}\sin^{2} x+\frac{6}{4}\cos^{2} x P_{TOT}=\frac{3}{2}(\sin^{2} x+\cos^{2} x) using the Pythagorean trigonometric identity P_{TOT}=\frac{3}{2} since we have eliminated x we can see that the total power does not vary with time. This is essential for keeping large generators and motors running smoothly.

no neutral current

the neutral current is the sum of the phase currents since R=1 I_{L1}=V_{L1}\,\! I_{L2}=V_{L2}\,\! I_{L3}=V_{L3}\,\! I_{N}=I_{L1}+I_{L2}+I_{L3}\,\! I_{N}=\sin x+\sin (x-\frac{2}{3} \pi)+\sin (x-\frac{4}{3} \pi) using angle subtraction formulae I_{N}=\sin x+\sin x\cos(\frac{2}{3} \pi)-\cos x\sin(\frac{2}{3} \pi)+\sin x\cos(\frac{4}{3} \pi)-\cos x\sin(\frac{4}{3} \pi) I_{N}=\sin x-\frac{1}{2}\sin x-\frac{\sqrt{3}}{2}\cos x-\frac{1}{2}\sin x+\frac{\sqrt{3}}{2}\cos x I_{N}=0\,\!

Star connected systems without neutral

Since we have shown that the neutral current is zero we can see that removing the neutral core will have no effect on the circuit, provided the system is balanced. In reality such connections are only generally used when the load on the three phases is part of the same piece of equipment (for example a three phase motor), as otherwise switching loads and slight imbalances would cause large voltage fluctuations.

Revolving Magnetic Field

Any polyphase system, by virtue of the time displacement of the currents in the phases, makes it possible to easily generate a magnetic field that revolves at the line frequency. Such a revolving magnetic field makes polyphase induction motors possible. Indeed, where induction motors must run on single-phase power (such as is usually distributed in homes), the motor must contain some measure to produce a revolving field, otherwise the motor cannot generate any stand-still torque and will not start. The field produced by a single-phase winding can provide energy to a motor already rotating, but without auxilary functions the motor will not accelerate from a stop when energized.

Conversion to other phase systems

Provided two voltage waveforms have at least some relative displacement on the time axis, other than a multiple of a half-cycle, any other polyphase set of voltages can be obtained by an array of passive transformers. Such arrays will evenly balance the polyphase load between the phases of the source system. A practical example is the Scott connection used to convert a three-phase system to a two-phase system with a displacment of 90 degrees between the phases. Such a two-phase system can produce a revolving magnetic field in a motor. Another practical example is the generation of higher-phase-order systems for large rectifier systems, which then produce a smoother DC output or may reduce the harmonic currents in the supply.

References

William D. Stevenson Jr., "Elements of Power Systems Analysis", 3rd ed. 1975, McGraw Hill, New York USA ISBN 0070612854

 

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