• Stabilizer, Spike Suppressor, Line Filter, Isolation Transformer ALL IN ONE
• Built-in Short Circuit & Overload Protection
• No interruption at output for small duration line interruptions/Brown-outs.
• Built-in Spike, Surge & RFI Suppression
• No electrical noise, as no moving parts or semi-conductors are used.
• 100 times faster than servo stabilizer.
• Can work at very low voltages on partial load.
•  

Quite often, line and load reactors are installed on AC drives without a solid understanding of why or what the positive and negative consequences are for adding this piece of hardware. The purpose of this document is to provoke some thought on the part of the person(s) responsible for the successful installation of the drive, and to provide some guidelines as to if, where and when a reactor is needed and what size reactor to use.

Let's first define what a reactor is. Essentially a reactor is an inductor. Physically it is simply a coil of wire that allows a magnetic field to form around the coil when current flows through it. When energized, it is an electric magnet with the strength of the field being proportional to the amperage flowing and the number of turns. A simple loop of wire is an air core inductor. More loops give a higher inductance rating. Quite often some ferrous material such as iron is added as a core to the winding. This has the effect of concentrating the lines of magnetic flux there by making a more effective Inductor.

Going back to basic AC circuit theory, an inductor has the characteristic of storing energy in the magnetic field and is reluctant to a change in current. The main property of a reactor is its inductance and is measured in henrys, millihenrys or microhenrys. In a DC circuit (such as that of the DC bus in an AC drive), an inductor simply limits the rate of change of current in the circuit since current in an inductor wants to continue to flow at the given rate for any instant in time. That is to say, an instantaneous increase or decrease in applied voltage will result in a slow increase or decrease in current. Conversely, if the rate of current in the inductor changes, a corresponding voltage will be induced. If we look at the equation V=L (di/dt) for an inductor where V is voltage, L is inductance and (di/dt) is the rate of change of current in amps per second, we can see that a positive rise in current will cause a voltage to be induced.

This induced voltage is opposite in polarity to the applied voltage and proportional to both the rate of rise of current and the inductance value. This induced voltage subtracts from the applied voltage thereby limiting the rate of rise of current. This inductance value is a determining factor of the reactance. The reactance is part of the total impedance for an AC circuit. The equation for the reactance of an inductor is X L = 2¶FL. Where X L is inductive reactance in Ohms, F is the applied frequency of the AC source and L is the inductance value of the reactor. As you can see, the reactance and therefore the impedance of the reactor is higher with a higher inductance value. Also, a given inductance value will have a higher impedance at higher frequencies. Thus we can say that in addition to limiting the rate of rise in current, a reactor adds impedance to an AC circuit proportional to both its inductance value and the applied frequency.

Like most medication there are side effects to using a reactor. Though these issues should not prevent the use of a reactor when one is required, the user should be aware of and ready to accommodate these effects. Since a reactor is made of wire (usually copper) wound in a coil, it will have the associated losses due to wire resistance. Also, if it is an Iron core inductor (as in the case of most reactors used in power electronics) it will have some “eddy current” loss in the core due to the changing magnetic field and the iron molecules being magnetically realigned. In general a reactor will add cost and weight, require space, generate heat and reduce efficiency.

Sometimes the addition of a line reactor can change the characteristics of the line you are connected to. Other components such as power factor correction capacitors and stray cable capacitance can interact with a line reactor causing a resonance to be set up. AC drives have/ exhibit a relatively good power factor and do not require the use of correction capacitors. In fact, power factor correction capacitors often do more harm than good where AC drives are present. For the most part, power factor correction capacitors should never be used with a drive. You may find that the addition of a reactor completes the required components for a line resonance where none previously existed, especially where power factor correction capacitors are present. In such cases either the capacitor or the inductor must be removed.

Furthermore, reactors have the effect of dropping some voltage, reducing the available voltage to the motor and or input of the motor drive.

One might ask; With all these side effects, why use a reactor? If you ask that question you might hear a whole slew of answers ranging from, “That's the way we always do it” to “I'd rather be safe than sorry.”

The fact is there are good reasons to install a reactor under certain conditions . Let's start with the input side of a drive.

A Reactor at the Input to reduce Harmonics :

As you may already know, most standard “six pulse” drives are nonlinear loads. They tend to draw current only at the plus and minus peaks of the line. Since the current waveform is not sinusoidal the current is said to contain “harmonics”. For a standard 3 phase input converter (used to convert AC to DC) using six SCR's or six diodes and a filter capacitor bank. The three-phase input current may contain as much as 85% or more total harmonic distortion. The reactor is expected to reduce the current distortion.