Phase-sequence indicator uses few passive components
Metodi Iliev, University of California—Berkeley; Edited by Brad Thompson and Fran Granville -- 7/6/2006
In a three-phase ac system, a power source with three wires delivers ac potentials of equal frequency and amplitudes with respect to a zero-potential wire, each shifted in phase by 120° from one wire to the next. Two possibilities exist for establishing a phase sequence. In the first, voltage on the second wire shifts by 120° relative to the first, and, in the second, a –120° shift occurs with respect to the first wire. Phase order determines the direction of rotation of three-phase ac motors and affects other equipment that requires the correct phase sequence: a positive 120° shift. You can use a few low-cost passive components to build a phase-sequence indicator.
Figure 1 shows a conceptual circuit that can detect both phase sequences. For certain component values, the following conditions apply: The voltages across R1 and C2 are equal—that is, their magnitudes and phases are the same—only when VS2 occurs exactly 120° ahead of VS1, which indicates the correct phase sequence. In this case, the voltage between points A and B is zero. Conversely, the voltages across C2 and R3 are equal only when VS2 is ahead of VS3 by 120°, which corresponds to a reversed sequence.
Referring to the phasor diagram in Figure
2, when the voltages across R1 and C2 are equal, VC1=–VR2, VC1+VR1=VS1, and VC2+VR2=VS2. The following equations satisfy these conditions: |VR1| = |VC2| =(½)| VS2|=(½)|VS1|, and |VC1| = |VR2| =cos(30°)|VS1| =cos(30°)|VS2|. You calculate the component values by solving the following equations: |XC1| = tan(60°)×R1=
and R2=tan(60°)×|XC2|, where XC=–j[1/(2π×f×C)], and f represents the frequency of the VS voltages.
Also, to ensure detection of a reversed phase sequence, C1=C3, and R1=R3; that is, the components in the third branch are identical to those in the first branch. The phase-sequence-detection circuit in Figure 3 eliminates the requirement for an accessible ground wire by adding resistors R4 and R5 that connect in parallel with the first and third branches. Eliminating the ground-wire requirement also dictates a ratio between |XC1+R1| and |XC2+R2|. For no current to flow to ground from Node G, the sum of currents in the branches must equal zero, and, if you disconnect Node G from ground, its potential with respect to ground is also zero.
A vector diagram of the currents shows that adding two currents, each with magnitudes equal to I3 and the same phases as VS1 and VS3, produces a summed current with the same magnitude and phase as I3; therefore, the total current at Node G is zero: I1+I2+I3+I1'+I3'=I1+I2+2×I3=0. To make the sum of the currents equal zero, R4=R5=|R1+XC1| = |R1–j[1/(2π×f×C1)]|. The two LEDs in Figure 3 indicate correct or reversed-phase sequence. When LED2 lights and LED1 remains dark, the voltage between nodes A and B is 0V, which corresponds to a correct phase sequence. A reversed-phase sequence lights LED1 while LED2 remains dark. The diodes connected in parallel with the LEDs protect against exceeding the LEDs' reverse-breakdown voltages, and resistors R6 and R7 limit forward currents through the LEDs. For greater sensitivity, you can replace the LEDs with high-input-impedance ac-detector circuits.
The circuit's final version includes indicators that show whether all three phases carry voltage. In the circuit in Figure 3, a phase that carries 0V lights both LEDs. Depending on your application, you can connect voltage-detection circuits comprising LEDs and protection diodes in series with current-limiting resistors between VS1, VS2, and VS3 and Node G. You can also use low-wattage neon lamps with appropriate series-current-limiting resistors.
When selecting components, ensure that their values conform to the following proportions. For an arbitrarily chosen value for C1, R1=R2=R3=1/(2π×f×C1×tan(60°)), C1=C3, C2=3C1, and R4=R5=2×R1. When you select a value for C1, the currents through the detection circuitry should be significantly lower than the currents through the branches, which excludes arbitrarily low values for C1.
© 2009, Reed Business Information, a division of Reed Elsevier Inc. All Rights Reserved.
