Description: The ratio of capacitors C1 and C2 determines the division. With a positive pulse applied to the base of Q1, assume that C1 = C2 and that C1 and C2 are discharged. When Q1 turns off, both C1 and C2 charge to 10 volts each through R3. On the next pulse to the base of Q1, C1 is again discharged but C2 remains charged to 10 volts. As Q1 turns off this time, C1 and C2 again charge. This time C2 charges to the peak point firing voltage of the Programmable Unijunction Transistor (PUT), causing it to fire. This discharges capacitor C2 and allows capacitor C1 to charge to the line voltage. The input and output frequency can be approximated by the equation (C1 = C2) C1. For a 10 kHz input frequency with an amplitude of 3 volts, the table shows the values for C1 and C2 needed to divide by 2 to 11. As soon as C2 discharges and C1 charges, the PUT turns off. The next cycle begins with another positive pulse on the base of Q1, which again discharges C1.
The described circuit employs capacitors C1 and C2 to create a voltage division mechanism influenced by the operation of a transistor Q1 and a Programmable Unijunction Transistor (PUT). The capacitors are initially in a discharged state, and when a positive pulse is applied to the base of Q1, both capacitors charge to a predetermined voltage, which is 10 volts in this scenario. The equal capacitance values of C1 and C2 facilitate a symmetrical charging and discharging process.
When Q1 is turned off, the capacitors undergo charging through resistor R3. The subsequent pulse at the base of Q1 causes C1 to discharge while C2 retains its charge. This sequence is crucial for the circuit's operation, as it allows C2 to reach the firing voltage of the PUT, leading to its activation. The firing of the PUT results in the discharge of C2, which in turn enables C1 to charge up to the line voltage, thereby creating a feedback loop that maintains the operation of the circuit.
The relationship between the input frequency and the capacitance values is critical for achieving the desired output frequency. The equation governing this relationship indicates that for a specific input frequency of 10 kHz and a voltage amplitude of 3 volts, certain capacitance values must be selected to ensure an effective division ratio, which is noted to be from 2 to 11 in the provided data. The operation of the circuit continues cyclically, with each cycle initiated by a positive pulse that prompts the discharge of C1, maintaining the overall functionality of the voltage division and timing mechanism.The ratio of capacitors Cl and C2 determines division. With a positive pulse applied to the base of Ql, assume that Cl = C2 and that Cl and C2 are discharged. When {31 turns off, both Cl and C2 charge to 10 volts each through R3. On the next pulse to the base of Ql, Cl is again discharged but C2 remains charged to 10 volts. As Ql turns off this time, Cl and C2 again charge. This time C2 charges to the peak point firing voltage of the PUT causing it to fire. This discharges capacitor C2 and allows capacitor Cl to charge to the line voltage. The input and output frequency can be approximated by the equation (Cl = C2) Cl For a 10 kHz input frequency with an amplitude of 3 volts, the table shows the values for Cl and C2 needed to divide by 2 to 11. As soon as C2 discharges and Cl charges, the PUT turns off. The next cycle begins with another positive pulse on the base of Ql which again discharges Cl.
If you require a small lamp that flashes for general use, there are numerous options available. Today, three lamp flasher circuits will be presented.
The three lamp flasher circuits can be designed using different components and configurations, each offering unique characteristics...
This page presents several transistor circuits that are not commonly found on other pages due to the absence of a specific topic. These circuits, however, illustrate particular points but lack detailed descriptions. An example of an RF amplifier circuit using...
A common-emitter transistor amplifier produces an output signal that is 180 degrees out of phase with the input signal, commonly referred to as an inverting amplifier. When the electrical path for amplifying the pulse signal is activated, this circuit functions...
The circuit diagram represents a simple radio utilizing one transistor and several passive components. The components C6 and L1 form a tank circuit that captures signals from the desired radio station. The diode D1, capacitor C2, and resistor R1 are...
This circuit is a low-frequency Wien bridge sinusoidal oscillator designed for the audio range, characterized by very low distortion, making it suitable for testing various audio equipment. The circuit has undergone thorough testing, and a printed circuit board (PCB) is...
Electrolytic capacitors are not required to generate a 1 cps frequency. When the silicon-controlled switch (SCS) is triggered, the 0.2 µF commutating capacitor deactivates the other capacitor and charges its gate capacitor to a negative potential. The gate capacitor charges...
This circuit utilizes three transistors (2SC945, 2C1815, or 2SC828) as the primary components, functioning as a typical low-noise transistor amplifier. It offers a gain of approximately 200 to 300 times and has a frequency response ranging from 50Hz to 100KHz....
This two-channel audio mixer utilizes 2N3904 transistors to create two preamplifiers. The first preamplifier is designed for high gain, suitable for microphone input, while the second preamplifier allows for control over the audio level input. The audio mixer requires a...
This circuit diagram illustrates a fully transistorized inverter capable of driving loads of up to 60W. Transistors Q1 and Q2 create a 50Hz astable multivibrator. The output from the collector of Q2 connects to the input of a Darlington pair...
We use cookies to enhance your experience, analyze traffic, and (if you allow) serve personalized ads.
By clicking Accept All, you agree to our use of cookies.
Learn more