How Does Current Flow in a Direct Coupled Oscillator Circuit?

In summary, the circuit in question involves two transistors and a speaker, and the current flow is controlled by the charging and discharging of a capacitor. The current splits into two branches, with the left path allowing current to flow from the emitter to the collector of the NPN transistor, while the right path blocks current until the PNP transistor is opened. The capacitor charges as the current flows through the resistor and the capacitor, and the speaker is used to discharge the capacitor. The circuit seems to be unstable and functions as an oscillator. This can be better understood by analyzing the dc voltages at various points in the circuit and their effect on the transistor currents.
  • #1
preet
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Could some one please help me understand the current flow in this circuit (electron flow theory)... specifically, how does the capacitor charge, and how do the two transistors open/close? So far this is what I think...

The current leaves the negative terminal, splits up into both branches... in the left path, the current goes into the emitter of the transistor (NPN) to the base, allowing current to flow from the emtter to the collector... much of the current returns to the positive terminal after leaving the collector, but some current takes the path through the resistor and the capacitor, charging it. In the right path, the current canot go past the transistor until it is opened by current flowing through the base to the emitter (PNP), but by this time, the capacitor is already charged and the current flowing through the circuit is practically nothing... this is as far as I get. I don't know how the current flows when the capacitor discharges...to discharge fully, energy has to be used up by the speaker.

So if anyone could explain if what I have is right, and what happens after the capacitor charges, i'd appreciate it. Thanks.

http://img114.echo.cx/img114/4327/circuit2cy.gif
 
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  • #2
preet said:
Could some one please help me understand the current flow in this circuit (electron flow theory)... specifically, how does the capacitor charge, and how do the two transistors open/close? So far this is what I think...

The current leaves the negative terminal, splits up into both branches... in the left path, the current goes into the emitter of the transistor (NPN) to the base, allowing current to flow from the emtter to the collector... much of the current returns to the positive terminal after leaving the collector, but some current takes the path through the resistor and the capacitor, charging it. In the right path, the current canot go past the transistor until it is opened by current flowing through the base to the emitter (PNP), but by this time, the capacitor is already charged and the current flowing through the circuit is practically nothing... this is as far as I get. I don't know how the current flows when the capacitor discharges...to discharge fully, energy has to be used up by the speaker.

So if anyone could explain if what I have is right, and what happens after the capacitor charges, i'd appreciate it. Thanks.

http://img114.echo.cx/img114/4327/circuit2cy.gif

I am more than rusty on this stuff, but I'll give it a shot. It appers to me to be a somewhat strange way to connect the speaker, but if this is what you were given, so be it. The capacitor will block the dc from flowing through it. If the voltage source is E then you should be able to figure out the dc voltage at the base of the PNP (also the voltage at the collector of the NPN), and at the base of the NPN, by considering base-emitter junction voltages. Since no dc flows through C, the two resistors will act as a voltage divider of the drop from the NPN collector to its base. So the dc voltage on the left side of C will depend on the ratio of the resistors. The base current of the PNP will depend on the size of those resistors (and how large E is), and the collector current of the PNP will be a large multiple of the PNP base current. The voltage at the collector of the PNP will be determined by the dc resistance of the speaker, because all of the PNP collector current has to flow there (not really a good idea to run dc through a speaker). When the capacitor is charged, the dc voltages will stabilize. Any small change in the base current of the PNP will produce a much larger change in the collector current and voltage, which will push ac through the capacitor, changing the base current of the NPN, changing the collector current. etc. Seems to be a rather unstable configuration. I guess that's why they call in an oscillator.

I suggest you start by finding the dc voltages at the various points in the circuit, and then think about the effect an ac component will have to alter those voltages.
 
  • #3


The direct coupled oscillator circuit is a type of electronic oscillator that uses two transistors to produce an oscillating signal. In this circuit, the two transistors act as amplifiers, with one amplifying the signal and the other providing feedback to sustain the oscillation.

Now, let's look at the current flow in this circuit. The current enters the circuit from the negative terminal of the power source and splits into two branches. In the left branch, the current flows through the emitter of the NPN transistor and into its base. This allows current to flow from the emitter to the collector, amplifying the signal. The amplified current then returns to the positive terminal of the power source.

In the right branch, the current cannot flow through the transistor until it is opened by current flowing through the base to the emitter of the PNP transistor. This current is provided by the feedback from the first transistor. As the current flows through the PNP transistor, it allows the capacitor to charge. The capacitor acts as a storage device for the energy and slowly charges up as the oscillation continues.

Once the capacitor is fully charged, it will discharge through the speaker, using up its energy and causing the capacitor to start charging again. This cycle repeats, creating the oscillation in the circuit.

In summary, the current flow in a direct coupled oscillator circuit is controlled by the transistors and the charging and discharging of the capacitor. By understanding the function of each component in the circuit, we can better understand how the current flows and how the oscillator produces its oscillating signal.
 

1. What is a direct coupled oscillator?

A direct coupled oscillator is a type of electronic circuit that generates an oscillating signal without the use of any external components such as transformers or capacitors. It consists of two or more active devices, typically transistors, that are connected directly to each other.

2. How does a direct coupled oscillator work?

A direct coupled oscillator works by using positive feedback to amplify and sustain an oscillating signal. The active devices in the circuit are biased to operate in their nonlinear region, causing the output signal to alternate between two states, resulting in an oscillation.

3. What are the advantages of a direct coupled oscillator?

Some advantages of a direct coupled oscillator include its simplicity, low cost, and stability. Since it does not require any external components, it is easy to design and has a lower cost. Additionally, it is less sensitive to temperature variations and can produce a stable output signal.

4. What are the applications of a direct coupled oscillator?

Direct coupled oscillators are commonly used in electronic devices such as radios, televisions, and computers. They are also used in electronic test equipment, signal generators, and sensors. Additionally, they are used in communication systems for frequency modulation and amplitude modulation.

5. How can the frequency of a direct coupled oscillator be controlled?

The frequency of a direct coupled oscillator can be controlled by adjusting the values of the components in the circuit, such as resistors and capacitors. Additionally, the frequency can be controlled by applying a voltage or current to the active devices in the circuit. This allows for a wide range of frequencies to be produced by a single oscillator circuit.

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