Presentation on theme: "Oscillations in an LC Circuit"— Presentation transcript:
1Oscillations in an LC Circuit AP Physics CMontwood High SchoolR. Casao
2When a charged capacitor is connected to an inductor as shown in the figure and the switch is then closed, oscillations will occur in the current and charge on the capacitor.If the resistance of thecircuit is zero, no energy isdissipated as joule heat andthe oscillations will persist.The resistance of the circuitwill be ignored.Assume that the capacitor has an initial charge Q and that the switch is closed at t = 0 s.
3It is easiest to describe what happens in terms of energy. When the capacitor is fully charged, the total energy U in the circuit is stored in the electric field of the capacitor and is equal toAt this time, the current is zero and there is no energy stored in the inductor.As the capacitor begins todischarge, the energy storedin its electric field decreases.The circuit behavior isanalogous to an oscillatingmass-spring system.
4At the same time, the current increases and some energy is now stored in the magnetic field of the inductor.Energy is transferred from theelectric field of the capacitor to themagnetic field of the inductor.When the capacitor is fullydischarged, it stores no energy.At this time, the current reachesits maximum value and all of the energy is now stored in the inductor.The process then repeats in the reverse direction.The energy continues to transfer between the inductor and capacitor indefinitely, corresponding to oscillations in the current and the charge.
5The potential energy stored in a stretches spring, 0 The potential energy stored in a stretches spring, 0.5·k·x2, is analogous to the potential energy stored in the capacitor,
6The kinetic energy of the moving mass, 0 The kinetic energy of the moving mass, 0.5·m·v2, is analogous to the energy stored in the inductor, 0.5·L·I2, which requires the presence of moving charges.
7All of the energy is stored as potential energy in the capacitor at t = 0 s because I = 0 A. All of the energy is stored as kinetic energy in the inductor, 0.5·L·Im2, where Im is the maximum current.
8In figure a, all of the energy is stored as electric potential energy in the capacitor at t = 0 s. In figure b, which is one-fourth of a period later, all of the energy is stored as magnetic energy 0.5·L·Imax2 in the inductor.
9In figure c, the energy in the LC circuit is stored completely in the capacitor, with the polarity of the plates now opposite to what it was in figure a.In figure d, all of the energy is stored as magnetic energy 0.5·L·Imax2 in the inductor.
10In figure e, the system has returned to the initial position, completing one oscillation. At intermediate points, part of the energy is potential energy and part is kinetic energy.At some time t after the switch is closed and the capacitor has a charge Q and the current is I.Both the capacitor and the inductor store energy, but the sum of the two energies must equal the total initial energy U stored in the fully charged capacitor at time t = 0 s.
11Since the circuit resistance is zero, no energy is dissipated as joule heat and the total energy must remain constant over time.Therefore:Differentiating the energy equation with respect to time and noting that Q and I vary with time:
13We can reduce the equation to a differential equation of one variable by using the following relationships:
14We can solve for the function Q by noting that the equation is of the same form as that of the mass-spring system (simple harmonic oscillator):where k is the spring constant, m is the mass, andThe solution for the equation has the general formwhere ω is the angular frequency of the simple harmonic motion, A is the amplitude of the motion (the maximum value of x), and is the phase constant; the values of A and depend on the initial conditions.
15Writing in the same form as the differential equation of the simple harmonic oscillator, the solution is:where Qm is the maximum charge of the capacitor and the angular frequency ω is given by:The angular frequency of the oscillation depends on the inductance and capacitance of the circuit.Since Q varies periodically, the current also varies periodically.
16Differentiating the harmonic oscillator equation for the LC oscillator with respect to time:
17To determine the value of the phase angle , examine the initial conditions. In the situation presented, when t = 0 s, I = 0 A, and Q = Qm.
18The time variation of Q and I are given by: The phase constant = 0.The time variation of Q and I are given by:where Im = ω·Qm is the maximumcurrent in the circuit.Graphs of Q vs. t and I vs. t:The charge on the capacitoroscillates between the extremevalues Qm and –Qm.
19Substituting the equations for the oscillating LC circuit into The current oscillates betweenIm and – Im.The current is 90º out of phasewith the charge.When the charge reaches anextreme value, the current is 0;when the charge is 0, the currenthas an extreme value.Substituting the equations forthe oscillating LC circuit intothe energy equations:
20Total energy:The equation shows that the energy of the system continuously oscillates between energy stored in the electric field of the capacitor and energy stored in the magnetic field of the inductor.
21When the energy stored in the capacitor has its maximum value, , the energy stored in the inductor is zero.When the energy stored in the inductor has its maximum value, 0.5·L·Im2, the energy stored in the capacitor is zero.The sum of the UC + UL is aconstant and equal to the totalenergy
22Since the maximum energy stored in the capacitor (when I = 0) must equal the maximum energy stored in the inductor (when Q = 0),Substituting this into the total energy equation:
23The total energy U remains constant only if the energy losses are neglected. In actual circuits, there will always be some resistance and so energy will be lost in the form of heat.Even when the energy losses due to wire resistance are neglected, energy will also be lost in the form of electromagnetic waves radiated by the circuit.
24An Oscillatory LC Circuit An LC circuit has an inductance of 2.81 mH and a capacitance of 9 pF. The capacitor is initially charged with a 12 V battery when the switch S1 is open and switch S2 is closed.S1 is then closed at the same timethat S2 is opened so that thecapacitor is shorted across thethe inductor.Find the frequency of theoscillation.
25Frequency for an LC circuit: What are the maximum values of charge on the capacitor and current in the circuit?Initial charge on the capacitor equals the maximum charge:
26Maximum current is related to the maximum charge: Determine the charge and current as functions of time.
27Energy Oscillations in the LC Circuit and the Mass-Spring System (harmonic oscillator)