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Show that the total energy is conserved during LC oscillations. - Physics

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प्रश्न

Show that the total energy is conserved during LC oscillations.

दीर्घउत्तर

उत्तर

Conservation of energy in LC oscillations: During LC oscillations in LC circuits, the energy of the system oscillates between the electric field of the capacitor and the magnetic field of the inductor. Although, these two forms of energy vary with time, the total energy remains constant. It means that LC oscillations take place in accordance with the law of conservation of energy.

Total energy,

U = UE + UB = `"q"^2/"2C" + 1/2 "Li"^2`

Let us consider 3 different stages of LC oscillations and calculate the total energy of the system.

Case I:

When the charge in the capacitor, q = Qm and the current through the inductor, i = 0, the total energy is given by

U = `"Q"_"m"^2/"2C" + 0 = "Q"_"m"^2/"2C"`

The total energy is wholly electrical.

Case II:

When charge = 0; current = Im, the total energy is

U = `0 + 1/2 "LI"_"m"^2 = 1/2 "LI"_"m"^2 = "L"/2 xx (("Q"_"m"^2)/"LC")`    .....since `"I"_"m" = "Q"_"m" omega = "Q"_"m"/sqrt"LC"`

`= "Q"_"m"^2/(2"C")`

The total energy is wholly electrical.

Case III:

When charge = q; current = i, the total energy is

U = `"q"^2/"2C" + 1/2 "Li"^2`

Since q = Qm cos ωt, i = `"bq"/"dt"` = Qmω sin ωt. The negative sign in current indicates that the charge in the capacitor in the capacitor decreases with time.

U = `("Q"_"m"^2 cos^2 omega"t")/("2C") + ("L"omega^2"Q"_"m"^2 sin^2 omega"t")/2`

`= ("Q"_"m"^2 cos^2 omega"t")/"2C" + ("L"^2"Q"_"m"^2 sin^2 omega"t")/"2LC"`    .....since `omega^2 = 1/"LC"`

U = `"Q"_"m"^2/"2C" (cos^2 omega"t" + sin^2 omega"t") = "Q"_"m"^2/"2C"`

From above three cases, it is clear that the total energy of the system remains constant.

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Oscillation in LC Circuits
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पाठ 4: Electromagnetic Induction And Alternating Current - Evaluation [पृष्ठ २६१]

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सामाचीर कलवी Physics - Volume 1 and 2 [English] Class 12 TN Board
पाठ 4 Electromagnetic Induction And Alternating Current
Evaluation | Q III. 25. | पृष्ठ २६१
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