BENEDICT electrical components Germany BENEDICT model BENEDICT price

BENEDICT electrical component is an energy conversion device that converts DC electrical energy into AC electrical energy with a specific frequency; the circuit it forms is called an oscillating circuit. Simply put, an oscillator is a frequency source, generally used in phase-locked loops. In detail, it is a device that can convert DC electrical energy into AC electrical energy on its own without external signal excitation. It is generally divided into two types: positive feedback and negative resistance. The term "oscillation" implies AC; the oscillator includes the process and function of transitioning from non-oscillating to oscillating. Such a device capable of completing the conversion from DC electrical energy to AC electrical energy can be called an "oscillator". Oscillators can be mainly divided into two types: harmonic oscillators and relaxation oscillators. They are electronic components used to generate repetitive electronic signals (usually sine waves or square waves). The circuit they form is called an oscillating circuit. It is an electronic circuit or device that can convert DC electricity into AC electrical signal output with a specific frequency. There are many types; classified by oscillation excitation method, they include self-excited oscillators and externally excited oscillators; classified by circuit structure, they include RC oscillators, LC oscillators, crystal oscillators, tuning fork oscillators, etc.; classified by output waveform, they include sine wave, square wave, sawtooth wave oscillators, etc. Widely used in the electronics industry, medical care, scientific research, and other aspects.

BENEDICT electrical component parameters

1. Nominal varistor voltage: refers to the voltage value across the varistor when a pulse current of specified duration passes through. 2. Voltage ratio: refers to the ratio of the voltage value generated by the current of the varistor to the voltage value generated by the current of the varistor. 3. Maximum clamping voltage: the peak voltage across the varistor under the maximum pulse peak current Ip that the varistor can withstand and under the specified waveform. 4. Residual voltage ratio: when the current passing through the varistor is a certain value, the voltage generated across it is called the residual voltage for this current value. The residual voltage ratio is the ratio of residual voltage to nominal voltage. 5. Surge current capacity: Surge current capacity, also known as surge current, refers to the maximum pulse current value allowed to pass through the varistor under specified conditions. 6. Leakage current: Leakage current, also known as standby current, refers to the current flowing through the varistor at the specified temperature and maximum DC voltage. 7. Voltage temperature coefficient: refers to the rate of change of the nominal voltage of the varistor within the specified temperature range, i.e., the relative change in voltage across the varistor when the temperature changes while the current passing through the varistor remains constant. 8. Current temperature coefficient: refers to the relative change in the current flowing through the varistor when the temperature changes while the voltage across the varistor remains constant. 9. Voltage nonlinearity coefficient: refers to the ratio of the static resistance value to the dynamic resistance value of the varistor under a given applied voltage. 10. Insulation resistance: refers to the resistance value between the lead wires of the varistor and the insulating surface of the resistor body. 11. Static capacitance: refers to the inherent capacitance of the varistor itself. 12. Rated power: the maximum power that causes a change in varistor voltage when operating at a specific ambient temperature. 24. Maximum impulse current: the maximum impulse current that causes a change in varistor voltage when the varistor is impacted by a specific pulse current once or twice.

BENEDICT electrical component types

Inductors can be made by winding conductive material, typically copper wire, around a magnetic core, or the magnetic core can be removed or replaced with ferromagnetic material. Core materials with higher permeability than air can confine the magnetic field more tightly around the inductor component, thereby increasing inductance. There are many types of inductors; most are made with enamel-coated coils wound around ferrite bobbins, while some shielded inductors place the coil completely inside the ferrite. The cores of some inductor components are adjustable, allowing the inductance value to be changed. Small inductors can be directly etched onto PCB boards using a method of laying out spiral traces. Small-value inductors can also be manufactured in integrated circuits using the same processes as for transistors. In these applications, aluminum interconnects are often used as conductive material. Regardless of the method, due to practical constraints, the most commonly used approach is a circuit called a "gyrator," which uses a capacitor and active components to exhibit the same characteristics as an inductor component. Inductor components used for blocking high frequencies are often constructed from a metal wire passing through a magnetic pillar or bead.

BENEDICT electrical component principle

In addition to the function of converting optical signals into electrical signals like a photodiode, a phototransistor also has the function of amplifying electrical signals. The appearance of a phototransistor is not much different from that of a general transistor. Generally, a phototransistor only leads out two terminals—the emitter and the collector—while the base is not led out. The casing also has a window to allow light to enter. To increase light exposure, the base region area is made large, while the emitter region is small; incident light is mainly absorbed by the base region. During operation, the collector junction is reverse-biased, and the emitter junction is forward-biased. When there is no light, the current flowing through the tube is the dark current Iceo = (1 + β) Icbo (very small), which is smaller than the penetration current of a general transistor; when there is light, a large number of electron-hole pairs are excited, causing the current generated at the base Ib to increase. At this moment, the current flowing through the tube is called photocurrent, and the emitter current Ie = (8 + β) Ib. It can be seen that a phototransistor has higher sensitivity than a photodiode.

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