Ques. What is mutual induction?
Ans. Mutual induction is the effect of one alternating current circuit upon another.
Fig. 2,677.—Measurement of self induction when the frequency is known. The apparatus required consists of a high resistance or electrostatic a.c. voltmeter, d.c. ammeter, and a non-inductive resistance. Connect the inductive resistance to be measured as shown, and close switch M, short circuiting the ammeter. Connect alternator in circuit and measure drop across R and across Xi. Disconnect alternator and connect battery in circuit, then open switch M and vary the continuous current until the drop across R is the same as with the alternating current, both measurements being made with the same voltmeter; read ammeter, and measure drop across Xi. Call the drop across Xi with alternating current E, and with direct current Ei, and the reading of the ammeter J. Then L = √E2 + Ei2 ÷ 2π f I. If the resistance Xi be known, and the ammeter be suitable for use with alternating current, the switch and R may be dispensed with.
Then L = √E2 - Xi2 Ii2 ÷ 2π f I, where Ii is the value of the alternating current. The resistance of the voltmeter should be high enough to render its current negligible as compared with that through Xi.
Ques. How is it caused?
Ans. It is due to the magnetic field surrounding a conductor cutting adjacent conductors and inducing back pressures therein.
This effect as a rule in ordinary installations is negligible.
Transpositions.—The effect of mutual induction between two circuits is proportional to the inter-linkage of the magnetic fluxes of the two lines. This in turn depends upon the proximity of the lines and upon the general relative arrangement of the conductors.