Description: In applications requiring long-range operation with infrared (IR) light sources and high system reliability, pulsed-mode operation of the IR source is essential. Enhanced operational reliability is achieved through synchronous detection of the photodetector current, as implemented in this circuit. The device PC-1 consists of an IR emitter and a phototransistor pair that detects the presence of an object obstructing the light transmission from the IR source to the phototransistor. Long-distance transmission is facilitated by pulsing the IR source with approximately 10 microsecond pulses at a 2 ms interval, delivering up to 350 mA through a 2N6027 oscillator.
The phototransistor current is amplified using 2N5249 and 2N5356 amplifiers to extend the operational range, allowing for the use of the H11A5, which is also pulsed by the 2N6027 as a synchronous detector. This configuration provides a fail-safe, noise-immune signal to the 2N5249 pair, forming a Schmitt-trigger output. The design is optimized for battery operation, prioritizing long battery life. It is important to note that an additional amplification stage driving the IR source can increase the range limited by the IR forward voltage by 5 to 10 times. Furthermore, a higher supply voltage for the IR source can potentially double this range. Currently, optoelectronics are predominantly utilized for transmitting electronic information via light beams. These applications encompass the use of optocouplers for information transfer between integrated circuit (IC) logic circuits and power circuits, between power lines and signal circuits, between telephone lines and control circuitry, as well as pulse-modulated systems that transmit information through air or fiber optics over considerable distances.
The circuit design incorporates several key components to achieve its objectives. The IR emitter, typically a high-efficiency LED or laser diode, is driven by the 2N6027 oscillator, which generates the required pulsed output. The choice of a 2N6027 is critical as it ensures that the pulsing can be finely controlled, enabling precise timing necessary for effective synchronous detection. The phototransistor, selected for its sensitivity to the specific wavelength of the IR light, operates in conjunction with the IR emitter to detect interruptions in the light path, thereby signaling the presence of an object.
Amplification stages are crucial for enhancing the signal received from the phototransistor. The 2N5249 and 2N5356 amplifiers are configured to provide high gain, ensuring that even weak signals can be effectively processed. The use of a Schmitt-trigger configuration helps to clean up the output signal, providing a sharp transition that is less susceptible to noise, which is particularly beneficial in environments with varying light conditions or electrical noise.
The overall design prioritizes battery efficiency, making it suitable for portable applications. The circuit can be powered by standard battery voltages, with considerations for minimizing current draw during idle states to extend operational life. The potential for range extension through additional amplification stages and increased supply voltage allows for flexibility in application, making this circuit suitable for a variety of optoelectronic communication systems, ranging from simple object detection to complex data transmission over long distances.When long ranges must be worked with IR light sources, and when high system reliability is required, pulsed-mode operation of the IRis required. Additional reliability of operation is attained by synchronously detecting the photodetector current, as this circuit does.
PC-1 is an IR and phototransistor pair which detect the presence of an object blocking the transmission of light from the IR to the phototransistor. Relatively long-distance transmission is obtained by pulsing theIR, with about 10-ftS pulses, at a 2-ms period, to 350 mA via the 2N6027 oscillator.
The phototransistor current is amplified by the 2N5249 and 2N5356 amplifier to further increase distance and allows use of the HllA5, also pulsed by the 2N6027, as a synchronous detector, providing a fail-safe, noise immune signal to the 2N5249 pair forrning a Schmitt-trigger output. This design was built for battery operation, with long battery life a primary consideration. Note that another stage of amplification driving the IR can boost the range limited by theIR VF, by 5 to 10 times.
A higher supply voltage for the IR can double this range. Today, optoelectronics are mostly used to transmit electronic information over light beams. These applications range from the use of optocouplers transmitting information between I C logic circuits and power circuits, between power lines and signal circuits, between telephone lines and control circuitry, to the pulse-modulated systems which transmit information through air or fiber optics over relatively great distances.
When the phototransistor is struck by infrared (IR) light, it begins to conduct, causing the voltage across a 1 MΩ resistor (chosen arbitrarily) and the phototransistor to drop from VCC to lower values. When this voltage falls below VCC/3, the...
Wireless infrared headphone transmitter. Audio input from PL1 frequency modulates the voltage-controlled oscillator (VCO) section of a 4046 phase-locked loop (PLL) chip. The VCO output drives Q1, a switching transistor, which in turn drives two infrared (IR) LEDs.
The wireless infrared...
This circuit employs a 15-kHz oscillator coil. When metal is removed from the energy field, the oscillator voltage is rectified and compared to a reference. A decrease in oscillator voltage activates comparator IC2, causing D4 (LED) to turn off.
L1 consists...
The metal detector circuit includes a fixed frequency oscillator, mixer, detector, detection oscillator, and power amplifier circuit. The fixed frequency oscillator circuit is composed of a ceramic filter (ZC), transistor (V1), resistors (R1 to R4), capacitor (C2), and other components....
This low-cost oscillator is consistently self-starting and capable of operating from over 1 Hz to 10 MHz, requiring only five components. The period of oscillation can be calculated using the relationship: P = 5 x 10^3 C seconds when C...
The XR-567 operates as a precision oscillator, providing two distinct square-wave outputs at pins 5 and 8, which are nearly in quadrature phase with one another. Due to the internal biasing configuration, the typical phase shift between the two outputs...
A blocking material monitoring circuit is presented. When the optical path is obstructed by the material, the phototransistor VT1 turns off, which subsequently turns off transistors VT2, VT3, and VT4. This arrangement is coupled to a flip-flop configuration. When the...
The electronic gong consists of an oscillator utilizing half of a 74C00 quad 2-input NAND gate, an active twin-T filter based on a TL081 operational amplifier, and an audio amplifier integrated circuit, such as the LM386N. Pulses generated by an...
The feedback control of the phototransistor in this optical detector helps negate the effects of varying ambient light sources. The output of a modulated visible-light LED is detected, amplified, buffered, and fed through a low-pass filter. Ambient light signals below...
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