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Question
Prove that energy is conserved during electromagnetic induction.
Solution
The mechanical energy of the spring-mass system is given by
E = `1/2 "mv"^2 + 1/2 "kx"^2` ......(1)
The energy E remains constant for varying values of x and v. Differentiating E with respect to time, we get
`"dE"/"dt" = 1/2 "m"("2v" "dv"/"dt") + 1/2"k" (2"x" "dx"/"dt") = 0`
or `"m" ("d"^2"x")/"dt"^2` + kx = 0 ......(2)
Since `"dx"/"dt" = "v" and "dv"/"dt" = ("d"^2"x")/"dt"^2`
This is the differential equation of the oscillations of the spring-mass system. The general solution of equation (2) is of the form
x(t) = Xm cos (ωt + φ) …… (3)
where Xm is the maximum value of x(t), ω, the angular frequency and φ, the phase constant. Similarly, the electromagnetic energy of the LC system is given by
U = `1/2 "Li"^2 + 1/2 (1/"C") "q"^2` = constant ....(4)
Differentiating U with respect to time, we get
`"dU"/"dt" = 1/2"L" ("2i" "di"/"dt") + 1/"C" ("2q" "dq"/"dt")` = 0
or `"L" ("d"^2"q")/"dt"^2 + 1/"C" "q" = 0` .....(5)
since i = `"dq"/"dt" and "di"/"dt" = ("d"^2"q")/"dt"^2` .....(5)
Equation (2) and (5) are proved the energy of electromagnetic induction is conserved.
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