* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Millmans Theorem - Wintec Learning
Integrating ADC wikipedia , lookup
Integrated circuit wikipedia , lookup
Topology (electrical circuits) wikipedia , lookup
Flexible electronics wikipedia , lookup
Josephson voltage standard wikipedia , lookup
Valve RF amplifier wikipedia , lookup
Wilson current mirror wikipedia , lookup
RLC circuit wikipedia , lookup
Operational amplifier wikipedia , lookup
Schmitt trigger wikipedia , lookup
Power electronics wikipedia , lookup
Resistive opto-isolator wikipedia , lookup
Switched-mode power supply wikipedia , lookup
Power MOSFET wikipedia , lookup
Current source wikipedia , lookup
Voltage regulator wikipedia , lookup
Opto-isolator wikipedia , lookup
Current mirror wikipedia , lookup
Surge protector wikipedia , lookup
DE5410 Class Note – Millman’s Theorem In electrical engineering, Millman's theorem (or the parallel generator theorem) is a method to simplify the solution of a circuit. Specifically, Millman's theorem is used to compute the voltage at the ends of a circuit made up of only branches in parallel. It is named after Jacob Millman, who proved the theorem. It permits any number of parallel branches consisting of voltage sources and impedances to be reduced to a single equivalent voltage source and equivalent impedance. Such multibranch circuits are frequently encountered in both electronics and power applications Figure 1 ek is the voltage generators and am the current generators. Ri be the resistances on the branches with no generator. Rk be the resistances on the branches with voltage generators. Rm be the resistances on the branches with current generators. Millman’s theorem states that the voltage at the ends of the circuit is given by: For a familiar three phase system this may be stated as follows: It can be proved by considering the circuit as a single supernode. Then, according to Ohm and Kirchhoff, "the voltage between the ends of the circuit is equal to the total current entering the supernode divided by the total equivalent conductance of the supernode". The total current is the sum of the currents flowing in each branch. The total equivalent conductance of the supernode is the sum of the conductance of each branch, since all the branches are in parallel. When computing the equivalent conductance all the generators have to be switched off, so all voltage generators become short circuits and all current generators become open circuits. That's why the resistances on the branches with current generators do not appear in the expression of the total equivalent conductance. V V V V V V V V