P12.15(a) Show that when the current in an isolated circuit element changes, the magnetic induction flux through that circuit element generated by that very current also changes. As a result of this, a "back' emf is generated. Show, using the Biot-Savart law to determine that the rate at which the flux changes with current is a constant (called 'self-inductance', represented by the letter L), dl that the induced emf is e=-L. dt

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PI2.15(a) Show that when the current in an isolated circuit element changes, the magnetic induction flux
through that circuit element generated by that very current also changes. As a result of this, a
"back' emf is generated. Show, using the Biot-Savart law to determine that the rate at which
the flux changes with current is a constant (called 'self-inductance', represented by the letter L),
dl
that the induced emf is e= -L.
dt
(b) Consider now two circuit coils placed next to each other. Let the number of turns in the first
coil be n and that in the second coil be n, and let the currents through them be, respectively,
I, and l. We shall denote by o, the flux through one turn of the coil i due to the current lj, with
i= 1, 2. A changing current in coil I induces an emf in the second: E =- M, where Ma is
dl,
dt
called the 'mutual inductance'. Prove that M21 = Mi2. which can be denoted by M.
(c) Prove that M= k/L4, where 0sks I and that this is a constant that depends only on the
geometrical elements of the two circuits.
(d) A magnetic field is given by B(z, t)= B
.Determine the emf it induces in a loop
Transcribed Image Text:PI2.15(a) Show that when the current in an isolated circuit element changes, the magnetic induction flux through that circuit element generated by that very current also changes. As a result of this, a "back' emf is generated. Show, using the Biot-Savart law to determine that the rate at which the flux changes with current is a constant (called 'self-inductance', represented by the letter L), dl that the induced emf is e= -L. dt (b) Consider now two circuit coils placed next to each other. Let the number of turns in the first coil be n and that in the second coil be n, and let the currents through them be, respectively, I, and l. We shall denote by o, the flux through one turn of the coil i due to the current lj, with i= 1, 2. A changing current in coil I induces an emf in the second: E =- M, where Ma is dl, dt called the 'mutual inductance'. Prove that M21 = Mi2. which can be denoted by M. (c) Prove that M= k/L4, where 0sks I and that this is a constant that depends only on the geometrical elements of the two circuits. (d) A magnetic field is given by B(z, t)= B .Determine the emf it induces in a loop
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