Low-light-level-drop-detector
This self-biasing configuration is useful whenever small changes in light level must be detected, such as when monitoring very low flow rates by counting drops of fluid. In this bias method, the photodarlington is bias stabilized by feedback from the collector, compensating for varying photodarlington gains and LED outputs. The 10 µF capacitor integrates the collector voltage feedback, while the 10 MΩ resistor provides a high base-source impedance to minimize effects on optical performance. The detector drop causes a momentary decrease in light reaching the chip, resulting in a temporary rise in collector voltage and generating an output signal. The initial light bias is small due to output power constraints on the LED and mechanical spacing system limitations. The change in light level is a fraction of this initial bias because of stray light paths and drop translucence. The high sensitivity of the photodarlington allows for acceptable output signal levels when biased in this manner, which contrasts with the unacceptable signal levels and bias point stability observed when using conventional biasing methods, such as leaving the base open and measuring the signal output across the collector bias resistor.
This self-biasing configuration employs a photodarlington in a feedback loop to maintain stable operating conditions while detecting minute variations in light intensity. By utilizing feedback from the collector, the circuit compensates for variations in the gain of the photodarlington and the output characteristics of the LED. The incorporation of a 10 µF capacitor serves to integrate the collector voltage feedback, smoothing out fluctuations and providing a stable reference for the system. The high-value 10 MΩ resistor connected to the base-source junction ensures minimal loading on the optical path, thereby preserving the integrity of the light signal being monitored.
In practical applications, such as low flow rate detection, the circuit responds to transient changes in light levels caused by the passage of fluid droplets. Each droplet momentarily obstructs the light reaching the photodarlington, leading to a brief increase in collector voltage, which is detected as an output signal. The design takes into account the constraints imposed by the LED's output power and the physical layout of the system, which can limit the initial light bias.
The system's sensitivity is crucial for detecting small changes, as the output signal generated from the photodarlington's response is directly related to the fluctuations in light intensity. This configuration is particularly advantageous compared to traditional methods, which may struggle with signal integrity and bias stability. In scenarios where the base of the photodarlington is left open, the resulting signal output across the collector bias resistor may not provide reliable data due to noise and instability, making the self-biasing approach a more effective solution for precise light level monitoring.This self-biasing configuration is useful any time srnall changes in light level must be detected, for example, when monitoring very low flow rates by counting drops of fluid. In this bias method, the photodarlington is de bias stabilized by feedback from the collector, compensating for different photodarlington gains and LED outputs.
The 10-I"F capacitor integrates the collector voltage feedback, and the 10-MO resistor provides a high base-source impedance to minimize effects on optical performance. The detector drop causes a momentary decrease in light reaching the chip, which causes collector voltage to momentarily rise, generating an output signal. The initial light bias is small because of output power constraints on the LED and mechanical spacing system constraints.
The change in light level is a fraction of this initial bias because of stray light paths and drop translucence. The high sensitivity of the photodarlington allows acceptable output signal levels when biased in this manner.
This compares with unacceptable signal levels and bias point stability when biased conventionally, i.e., base open and signal output across the collector bias resistor. 🔗 External reference
This self-biasing configuration employs a photodarlington in a feedback loop to maintain stable operating conditions while detecting minute variations in light intensity. By utilizing feedback from the collector, the circuit compensates for variations in the gain of the photodarlington and the output characteristics of the LED. The incorporation of a 10 µF capacitor serves to integrate the collector voltage feedback, smoothing out fluctuations and providing a stable reference for the system. The high-value 10 MΩ resistor connected to the base-source junction ensures minimal loading on the optical path, thereby preserving the integrity of the light signal being monitored.
In practical applications, such as low flow rate detection, the circuit responds to transient changes in light levels caused by the passage of fluid droplets. Each droplet momentarily obstructs the light reaching the photodarlington, leading to a brief increase in collector voltage, which is detected as an output signal. The design takes into account the constraints imposed by the LED's output power and the physical layout of the system, which can limit the initial light bias.
The system's sensitivity is crucial for detecting small changes, as the output signal generated from the photodarlington's response is directly related to the fluctuations in light intensity. This configuration is particularly advantageous compared to traditional methods, which may struggle with signal integrity and bias stability. In scenarios where the base of the photodarlington is left open, the resulting signal output across the collector bias resistor may not provide reliable data due to noise and instability, making the self-biasing approach a more effective solution for precise light level monitoring.This self-biasing configuration is useful any time srnall changes in light level must be detected, for example, when monitoring very low flow rates by counting drops of fluid. In this bias method, the photodarlington is de bias stabilized by feedback from the collector, compensating for different photodarlington gains and LED outputs.
The 10-I"F capacitor integrates the collector voltage feedback, and the 10-MO resistor provides a high base-source impedance to minimize effects on optical performance. The detector drop causes a momentary decrease in light reaching the chip, which causes collector voltage to momentarily rise, generating an output signal. The initial light bias is small because of output power constraints on the LED and mechanical spacing system constraints.
The change in light level is a fraction of this initial bias because of stray light paths and drop translucence. The high sensitivity of the photodarlington allows acceptable output signal levels when biased in this manner.
This compares with unacceptable signal levels and bias point stability when biased conventionally, i.e., base open and signal output across the collector bias resistor. 🔗 External reference