Three-phase electric power is a common method of alternating-current electric power generation, transmission, and distribution.  A three-phase system is generally more economical than others because it uses less conductor material to transmit electric power than equivalent single-phase or two-phase systems at the same voltage.
In a three-phase system, three circuit conductors carry three alternating currents (of the same frequency) which reach their instantaneous peak values at different times. Taking one conductor as the reference, the other two currents are delayed in time by one-third and two-thirds of one cycle of the electric current. This delay between phases has the effect of giving constant power transfer over each cycle of the current and also makes it possible to produce a rotating magnetic field in an electric motor.
* V_a(t)=V_p \sin(\omega\,t-\tfrac{2}{3}\pi)=V_p (-\tfrac{1}{2}\sin \omega t-\tfrac{\sqrt{3}}{2}\cos\omega t)
* V_b(t)=V_p \sin(\omega\,t)
* V_c(t)=V_p \sin(\omega\,t+\tfrac{2}{3}\pi)=V_p (-\tfrac{1}{2}\sin \omega t+\tfrac{\sqrt{3}}{2}\cos\omega t)

And you will find V_a(t)+V_b(t)+V_c(t)=0.

Three-phase systems may have a neutral wire. A neutral wire allows the three-phase system to use a higher voltage while still supporting lower-voltage single-phase appliances.
[li]The phase currents tend to cancel out one another, summing to zero in the case of a linear balanced load. This makes it possible to eliminate or reduce the size of the neutral conductor; all the phase conductors carry the same current and so can be the same size, for a balanced load.
Power transfer into a linear balanced load is constant, which helps to reduce generator and motor vibrations.
Three-phase systems can produce a magnetic field that rotates in a specified direction, which simplifies the design of electric motors.

The following simulation let you play with such 3 phase electric power system, power source and load either in Y or \Delta connection mode.
Use checkbox to select AC Y mode (AC \Delta mode) or R Y mode (R \Delta mode)
For AC Y mode:
Phase voltage referer to V[sub]RN[/sub]=V[sub]a[/sub],V[sub]SN[/sub]=V[sub]b[/sub],V[sub]TN[/sub]=V[sub]c[/sub],
Line voltage referer to V[sub]RS[/sub]=V[sub]a[/sub]-V[sub]b[/sub],V[sub]ST[/sub]=V[sub]b[/sub]-V[sub]c[/sub],V[sub]TR[/sub]=V[sub]c[/sub]-V[sub]a[/sub].

Y-connected sources and loads always have line voltages greater than phase voltages, and line currents equal to phase currents. If the Y-connected source or load is balanced, the line voltage will be equal to the phase voltage times the square root of 3.

V_a-V_b=V_p (-\tfrac{3}{2}\sin \omega t-\tfrac{\sqrt{3}}{2}\cos\omega t)=\sqrt{3}\,V_p (-\tfrac{\sqrt{3}}{2}\sin \omega t-\tfrac{1}{2}\cos\omega t)=\sqrt{3} V_p \sin(\omega\,t-\tfrac{5}{6}\pi)

translate strings in simulation to different language format before download
Full screen applet or Problem viewing java?Add to exception site list
Press the Alt key and the left mouse button to drag the applet off the browser and onto the desktop. This work is licensed under a Creative Commons Attribution 2.5 Taiwan License
Download EJS jar file(1136.1kB):double click downloaded file to run it. (33 times by 26 users) , Download EJS source View EJS source