Capacitors, Magnetic Circuits, and Transformers is a free introductory textbook on the physics of capacitors, coils, and transformers. See the editorial for more information.... |
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Resistance and Self-Inductance
Figure 1-7 shows a schematic diagram of an R-L circuit. When there is current in such a circuit, the self-inductance has energy that is stored electro-magnetically. The electrical energy in the resistance is converted into thermal energy. The mathematical relationships in this kind of circuit are very similar to those in the mechanical system involving mass and friction.
In Fig. 1-7 the applied voltage V is constant and equals two components
eR = iR, the resistance drop Equation 1-37 can be rewritten as
and the power is expressed by
The electric power converted into heat is Ri2 and that stored electro-magnetically is Li di/dt. The energy relationship is expressed by the following
If the initial conditions are i = 0 when t = 0, then Eq. 1-38 becomes
where Li2/2 represents the energy stored in the self-inductance. If the initial conditions are such that i = 0 when t = 0, the current in the R-L circuit is expressed by
The reciprocal L/R of the constant term in the exponent of Eq. 1-40 is the time constant t. It corresponds to the time constant M/RF in the mechanical system.
A comparison of Eq. 1-34 with 1-40 shows that if voltage is taken as analogous to force and electrical resistance as analogous to frictional resistance in the mechanical system, current corresponds to velocity and self-inductance to inertia. Curves similar to those shown in Fig. 1-8 would portray the relationships for the mechanical system. Thus the curve of current i vs time could be used to relate the velocity v to time in the mechanical system. Similarly, the curve of pφ vs time could be used to represent the mechanical power Mv dv/dt, which stores energy in the moving mass of the mechanical system. The energy 1/2Mv2 stored in the mass could also be represented as a function of time by the curve of WL vs time.
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