Can LC Oscillations Be Generated Using a DC Source?

In summary, the conversation discusses a circuit with an inductor, uncharged capacitor, and ideal battery in series. When the circuit is switched on at t=0, the following events occur: the current is initially at its maximum, the battery charges the capacitor causing the current to decrease, the inductor senses the change in current and sets up a back EMF, which causes the current to decay from exponential decay to sinusoidal decay, the capacitor reaches its maximum charge, the back EMF from the inductor vanishes as the current decreases, the electric field energy transforms to magnetic field energy causing the capacitor to discharge to the inductor, the back EMF from the inductor causes the current to grow in the opposite direction, the charge
  • #1
saubhik
31
0

Homework Statement



Suppose we have a circuit with the inductor, uncharged capacitor, ideal battery with emf E all in series. At t=0, the circuit is switched on. The following takes place sequentially:
1. Current at t=0 is max. Battery charges capacitor, current decreases.
2. inductor senses change in current, sets up back emf, decreasing the rate of current decay from exponential decay to a sinusoidal decay.
3. capacitor gets charged to max i.e. C*E. Current falls to 0.
4. inductor's back emf vanishes as current vanishes.
5. electric field energy tends to transform to magnetic field energy. Thus, capacitor discharges to the inductor.
6. the back emf set by inductor again describes the rate of change of current growth in opposite direction.
7. charge on capacitor falls to 0 and current reaches its max value, this time in opposite.
8. capacitor gets charged again and the whole process gets repeated in opposite direction for the next half cycle and so on.

Homework Equations



from above analysis, current and charge have phase diff of 90. Both sinusoidal functions.
max charge is C*E and max current is (resonant angular frequency)*(max charge).

We can get these by solving the differential equation obtained using KVL.

The Attempt at a Solution



we have an alternating current from a d.c. voltage.
Please see if my analysis is correct! also please point out if i am lacking in finer details...
I didn't know we could get AC from a DC supply.
Also i didnt find any transient characteristics of this circuit? which circuits have transient solutions?
 
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  • #2
The inductor in the series circuit is not going to allow "Current at t=0 is max". So you've got a problem at step 1.

Have a look http://en.wikipedia.org/wiki/RLC_circuit" .
 
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  • #3
yah...
that's right.
So the equations don't hold for t=0?
is that the DC transcience?

what then happens exactly at t=0; how to express this mathematically?
 
  • #4
saubhik said:
yah...
that's right.
So the equations don't hold for t=0?
is that the DC transcience?

what then happens exactly at t=0; how to express this mathematically?

You just need the right equations. Write out the differential equation for the circuit and solve for the "step response". It's a second order system, characterized by containing two different passive energy storage components (the capacitor and the inductor), so you get a second order differential equation, which means it'll have characteristics like damping factors and resonance. The web page I linked to in my post above has the details.
 
  • #5


Your analysis is correct. In this circuit, the inductor and capacitor act as a resonant circuit, with the inductor providing the back emf to counter the decrease in current and the capacitor storing the energy transferred between the electric and magnetic fields. This results in a sinusoidal oscillation of current and charge.

Regarding your question about getting AC from a DC supply, it is possible through the use of an inductor as it allows for the creation of a varying magnetic field, which in turn induces a varying voltage. This is known as an AC-DC converter.

As for the transient characteristics, this circuit does have a transient solution as it takes time for the current to reach its maximum and for the capacitor to fully charge. The transient solution can be found by solving the differential equation obtained using KVL.

Circuits with transient solutions are those that exhibit a time-dependent behavior, such as in this case where the current and charge vary over time. Other examples include RC circuits, RL circuits, and RLC circuits. These circuits have a transient solution as they take time to reach their steady-state behavior.
 

Related to Can LC Oscillations Be Generated Using a DC Source?

1. What is an LC oscillator with a DC source?

An LC oscillator with a DC source is a circuit that uses a combination of an inductor (L) and a capacitor (C) to generate an alternating current (AC) signal from a direct current (DC) source. The inductor and capacitor work together to create an oscillation or back-and-forth motion of the current, resulting in a sinusoidal output.

2. How does an LC oscillator with a DC source work?

The DC source supplies a constant voltage, which charges the capacitor. As the capacitor charges, it creates a magnetic field around the inductor, storing energy in the form of an electric current. When the capacitor is fully charged, the current stops flowing and the magnetic field collapses, causing the current to reverse direction. This cycle repeats, creating an oscillation of the current between the inductor and capacitor.

3. What are the applications of LC oscillators with DC sources?

LC oscillators with DC sources are commonly used in electronic circuits as a source of radio frequency (RF) signals. They are also used in electronic devices such as radios, televisions, and computers to generate clock signals and for frequency modulation (FM) and amplitude modulation (AM) in communication systems.

4. What are the advantages of using an LC oscillator with a DC source?

One of the main advantages of using an LC oscillator with a DC source is its simplicity and low cost. It also has a wide frequency range and can generate stable and precise signals. Additionally, the output frequency can be easily adjusted by changing the values of the inductor and capacitor in the circuit.

5. How can I improve the performance of an LC oscillator with a DC source?

To improve the performance of an LC oscillator with a DC source, you can use high-quality components and ensure proper circuit design. Adding a buffer amplifier can also help to improve the output signal strength and stability. Additionally, using a feedback mechanism or a phase-locked loop (PLL) can help to reduce frequency drift and maintain a constant output frequency.

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