JoVE Logo

S'identifier

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by

Equation1

When the switch is closed, the capacitor begins to discharge, producing a current in the circuit. The current, in turn, creates a magnetic field in the inductor. The net effect of this process is a transfer of energy from the capacitor, with its diminishing electric field, to the inductor, with its increasing magnetic field. When the capacitor is completely discharged and all the energy is stored in the inductor's magnetic field, the current in the inductor is at its maximum value. At this instant, the energy stored in the inductor is given by

Equation2

At an arbitrary time, the capacitor charge and current varies with time. Therefore the total energy U in the circuit is given by

Equation3

Since there is no resistance in the circuit, no energy is lost through Joule heating; the energy in circuit remains conserved. After reaching the maximum current in the inductor, the current continues to transport charge between the capacitor plates, thereby recharging the capacitor. Since the inductor resists a change in current, current continues to flow, even though the capacitor is discharged. This continued current causes the capacitor to charge with opposite polarity. If there is no energy dissipation, charge on the capacitor plates continues to change polarity indefinitely, causing electrical oscillations. The angular frequency of these oscillations in the circuit is given by

Equation4

Tags

LC CircuitOscillationsElectric FieldMagnetic FieldCapacitor ChargeEnergy TransferCurrentInductorEnergy ConservationElectrical OscillationsAngular Frequency

Du chapitre 31:

article

Now Playing

31.11 : Oscillations In An LC Circuit

Inductance

2.1K Vues

article

31.1 : Inductance mutuelle

Inductance

2.2K Vues

article

31.2 : Auto-inductance

Inductance

2.3K Vues

article

31.3 : Calcul de l’auto-inductance

Inductance

253 Vues

article

31.4 : Inductances

Inductance

5.4K Vues

article

31.5 : Énergie dans un champ magnétique

Inductance

2.2K Vues

article

31.6 : Énergie stockée dans un câble coaxial

Inductance

1.3K Vues

article

31.7 : RL Circuits

Inductance

2.4K Vues

article

31.8 : Croissance et décroissance du courant dans les circuits RL

Inductance

3.6K Vues

article

31.9 : Comparaison entre les circuits RL et RC

Inductance

3.6K Vues

article

31.10 : LC Circuits

Inductance

2.3K Vues

article

31.12 : Circuits de la série RLC

Inductance

2.8K Vues

article

31.13 : Circuit RLC en tant qu’oscillateur amorti

Inductance

806 Vues

JoVE Logo

Confidentialité

Conditions d'utilisation

Politiques

Recherche

Enseignement

À PROPOS DE JoVE

Copyright © 2025 MyJoVE Corporation. Tous droits réservés.