igus electrical components Germany igus model igus price

igus electrical components refer to electronic components that generate resonant frequencies. Common types include quartz crystal resonators and ceramic resonators. They function to generate frequencies, featuring stability and good anti-interference performance, and are widely used in various electronic products. The frequency accuracy of quartz crystal resonators is higher than that of ceramic resonators, but the cost is also higher. Resonators mainly serve the role of frequency control; all electronic products involving frequency transmission and reception require resonators. Based on their physical form, resonators can be divided into two types: through-hole and surface-mount.

igus electrical component principle

The working principle of a discharge tube is gas gap discharge. i When a certain voltage is applied between the two poles of the discharge tube, an uneven electric field is generated between the poles: under the action of this electric field, the gas inside the tube begins to ionize. When the external voltage increases to the point where the field strength between the poles exceeds the insulation strength of the gas, the gap between the two poles breaks down due to discharge, transforming from an insulating state to a conductive state. After conduction, the voltage between the two poles of the discharge tube is maintained at the residual voltage level determined by the discharge arc channel. This residual voltage is generally very low, thereby protecting electronic equipment connected in parallel with the discharge tube from overvoltage damage.

igus electrical component characteristics

The main parameters characterizing resistor characteristics include nominal resistance and its tolerance, rated power, load characteristics, and temperature coefficient of resistance. Load characteristics: When the ambient operating temperature is below tR, the resistor must not exceed its rated power. When exceeding tR, the load power must be reduced. Each type of resistor has specified load characteristics. Additionally, the allowable load decreases under low atmospheric pressure. Under pulse load conditions, the average pulse power is far lower than the rated power, and separate specifications usually apply. Within the specified ambient temperature range, the average relative change in resistance for every 5℃ change in temperature is expressed in ppm/℃. In addition to the above parameters, other technical indicators include nonlinearity (the degree to which the current-voltage characteristic deviates from a linear relationship), voltage coefficient (the relative rate of change in resistance per volt change in applied voltage), current noise (the ratio of the RMS value of the noise potential generated by current flow within the resistor body to the test voltage, expressed by the current noise index), high-frequency characteristics (the curve showing the decrease in resistance as operating frequency increases due to distributed capacitance and inductance within the resistor body), and long-term stability (the process of irreversible changes in resistance caused by environmental conditions during long-term use or storage).

igus electrical component structure

A bipolar transistor consists of three differently doped semiconductor regions: the emitter region, the base region, and the collector region. In an NPN type transistor, these regions are N-type, P-type, and N-type semiconductors, respectively, while in a PNP type transistor, they are P-type, N-type, and P-type semiconductors, respectively. Each semiconductor region has a lead terminal, typically denoted by the letters E, B, and C for the emitter, base, and collector, respectively. The base is physically located between the emitter and the collector and is made of lightly doped, high-resistivity material. The collector surrounds the base region. Since the collector junction is reverse-biased, it is difficult for electrons to be injected from here into the base region, resulting in a common-base current gain of approximately 4, while the common-emitter current gain achieves a larger value. From the cross-sectional diagram of a typical NPN type bipolar transistor on the right, it can be seen that the area of the collector junction is larger than that of the emitter junction. Furthermore, the emitter has a relatively high doping concentration. Under normal circumstances, the regions of a bipolar transistor are not symmetric in physical properties or geometric dimensions. Assuming the transistor connected in the circuit is in the forward active region, swapping the connections of the collector and emitter in the circuit will cause the transistor to leave the forward active region and enter the reverse active region. The internal structure of the transistor determines that it is suitable for operation in the forward active region, so the common-base and common-emitter current gains in the reverse active region are much smaller than when the transistor is in the forward active region. This functional asymmetry is fundamentally due to the different doping levels of the emitter and collector. Therefore, in an NPN type transistor, although both the collector and emitter are N-type doped, their electrical properties and functions are completely interchangeable. The emitter region has the highest doping concentration, followed by the collector region, and the base region has the lowest doping concentration. Additionally, the physical dimensions of the three regions differ; the base region is very thin, and the collector area is larger than the emitter area. Due to this material structure of the bipolar transistor, a reverse bias can be provided to the collector junction, provided that this reverse bias is not excessive enough to damage the transistor. The purpose of heavy doping of the emitter is to increase the efficiency of electron injection from the emitter into the base region, thereby achieving the highest possible current gain. In the common-emitter configuration of a bipolar transistor, small changes in the voltage applied across the base and emitter terminals cause significant changes in the current between the emitter and collector. Utilizing this property, input current or voltage can be amplified. By treating the base of the bipolar transistor as the input terminal and the collector as the output terminal, this two-port network can be analyzed using Thevenin's theorem. Based on equivalent principles, the bipolar transistor can be viewed as a voltage-controlled current source or as a current-controlled voltage source. Furthermore, looking into the left side of the two-port network, the input impedance at the base is reduced to the base resistance, thus lowering the requirements for the loading capacity of the preceding stage circuit.

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