COMMON MODE CHOKE THEORY
A common mode choke may be used to reduce a type of electrical noise known as common mode noise.
Electro-Magnetic Interference (E.M.I.)
E.M.I. in the circuit’s environment is one source of electrical noise. E.M.I. induces Common Mode Choke or couples unwanted electrical signals into the circuit. It is Product Page desirable to filter out the unwanted noise signals without significantly affecting the desired signal. Environmental sources Power Inductors, Chokes of E.M.I. often create an independent return path (ground path) & Reactors FAQs for the electrical noise signals. The return path of the desired signal is a different path. Because there are two different return paths, a Common Mode Choke can be used to significantly block (hence reduce) the unwanted noise signal (at the load) without significant reduction in the desired signal.
A.C. Power Lines
A.C. Power Lines provide a good example. They are known to carry significant levels of electrical noise. Their long length gives environmental E.M.I. ample opportunity to generate unwanted electrical noise into the power lines.
Figure 2 below illustrates an application without a Common Mode Choke.
In the example above, the power line voltage, “Vs”, causes current, “Iz”, to flow through the load, “Z”. At any non-zero instance, Current “Iz” flows into “Z” through one power line wire and returns through the other power line wire. E.M.I. voltage, “Vnc1”, causes current “Inc1”, to flow through the load “Z”. Similarly, E.M.I. voltage, Vnc2 causes current “Inc2” to flow through the load “Z”. Because the E.M.I is generating both “Vnc1” and “Vnc2” – the two voltages tend to be in phase. There is very little current flow between them. Current “Inc1” does not flow through both power line wires. It flows through one power line wire and through the ground path. Similarly, current “Inc2” does not flow through both power line wires. It flows through one power line wire and through the ground path. In this example only “Vnc1” produces electrical noise across load “Z” because the “Vnc2” end of “Z” is grounded. In practice, the effective ground point could occur somewhere between the two ends of load “Z”.
Figure 3 below illustrates the same application with a Common Mode Choke.
The common mode choke has two windings. Each winding of the common mode choke is inserted between the end of a power line wire and the load.
In the example above, the power line voltage, “Vs”, causes current, “Iz”, to flow through the load, “Z”. At any non-zero instance, Current “Iz” flows into “Z” through one power line wire and returns through the other power line wire. E.M.I. voltage, “Vnc1”, causes current “Inc1”, to flow through the load “Z”. Similarly, E.M.I. voltage, Vnc2 causes current “Inc2” to flow through the load “Z”. Because the E.M.I is generating both “Vnc1” and “Vnc2” – the two voltages tend to be in phase. There is very little current flow between them. Current “Inc1” does not flow through both power line wires. It flows through one power line wire and through the ground path. Similarly, current “Inc2” does not flow through both power line wires. It flows through one power line wire and through the ground path. In this example only “Vnc1” produces electrical noise across load “Z” because the “Vnc2” end of “Z” is grounded. In practice, the effective ground point could occur somewhere between the two ends of load “Z”.
Figure 3 below illustrates the same application with a Common Mode Choke.
The common mode choke has two windings. Each winding of the common mode choke is inserted between the end of a power line wire and the load.
The inductance of Winding A restricts (reduces) the flow of current “Inc1” (when compared to Figure 1), thereby reducing the noise voltage across “Z”. Similarly the inductance of winding B restricts (hence reduces) the flow of current “Inc2”. Windings A and B have the same number of turns. The ampere-turns created by Current “Iz” (but excluding any “Inc1” current component) flowing through winding A is cancelled by the opposing ampere-turns created by current “Iz” flowing through winding B. Ideally, the cancellation results in zero inductance and no restriction (no reduction) of current “Iz”. “Iz” produces the same voltage across load “Z” as it does in Figure 1. In practice this will not be true. The common mode choke will have some leakage flux between windings A and B hence incomplete cancellation. Windings A and B will have some winding resistance. Both of these will have some effect on “Iz” (reduces “Iz”).
In contrast, the load current “Iz” flowing through both Winding A and Winding B of the differential choke shown in Figure 1 do not cancel, hence “Iz” will be restricted (reduced). Differential chokes are useful when the electrical noise frequencies are much higher than the operating frequencies. The higher choke impedance at the high frequencies block the electrical noise while having a tolerable effect at the operating frequencies.
Some common mode chokes are intentionally designed to have significant leakage inductance. The leakage inductance acts in series with the load hence the leakage inductance provides differential noise filtering. One common mode choke functions like the combined chokes shown in Figure 1 but may differ in levels.
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