
ELEKTROSVITNOVE electrical components Germany ELEKTROSVITNOVE model ELEKTROSVITNOVE price
ELEKTROSVITNOVE electrical components are energy conversion devices that convert DC electrical energy into AC electrical energy with a specific frequency; the circuit they form 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 alternating current; an oscillator includes the process and function of transitioning from non-oscillating to oscillating. Capable of completing the conversion from DC
- SKU
- _P004836961
- Category
- Electrical and Electronic Components
- Brand
- ELEKTROSVITNOVE
- Tags
- Connectors / Cable / Switch / Relay / Controller / Germany ELEKTROSVITNOVE
ELEKTROSVITNOVE electrical component principle
It is a contactless switching device with relay characteristics that uses semiconductor devices to replace traditional electrical contacts as the switching mechanism. A single-phase solid-state relay is a four-terminal active device, with two input control terminals and two output terminals. There is optical isolation between the input and output. When a DC or pulse signal is applied to the input terminal and reaches a certain current value, the output terminal switches from the off state to the on state. AC solid-state relays are classified by switching method into zero-crossing conduction type and random conduction type; by output switching element into triac output type and anti-parallel SCR type. By installation method, they are divided into pin-type for printed circuit boards and chassis-mounted type fixed on metal baseplates. Solid-state relays can be divided into zero-voltage type and phase-control type based on the triggering mode.
ELEKTROSVITNOVE 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 derated. Each type of resistor has specified load characteristics. In addition, the allowable load is correspondingly reduced under low atmospheric pressure. Under pulse load, 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 11℃ change in temperature is expressed in ppm/℃. In addition to the above parameters, there are other technical indicators such as nonlinearity (the degree to which the current versus applied 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 the operating frequency increases due to the influence of distributed capacitance and inductance within the resistor body), and long-term stability (the process of irreversible change in resistance value due to environmental conditions during long-term use or storage).
ELEKTROSVITNOVE electrical component principle
P-type semiconductors are formed by doping intrinsic semiconductors (a completely pure, structurally perfect semiconductor crystal) with a small amount of trivalent impurity elements, such as boron. Since a boron atom has only three valence electrons, it forms covalent bonds with surrounding silicon atoms. Due to the lack of one electron, a vacancy is created in the crystal. When an electron on an adjacent covalent bond gains energy, it may fill this vacancy, causing the boron atom to become an immobile negative ion, while the original silicon atom's covalent bond forms a hole due to the missing electron. However, the entire semiconductor remains neutral. In this P-type semiconductor, conduction is primarily by holes, which are the majority carriers, while free electrons are the minority carriers. The principle of forming N-type semiconductors is similar to that of P-type. Pentavalent atoms, such as phosphorus, are doped into the intrinsic semiconductor. After doping, they form covalent bonds with silicon atoms, generating free electrons. In N-type semiconductors, electrons are the majority carriers, and holes are the minority carriers. Therefore, doping trivalent and pentavalent impurity elements into two different regions of an intrinsic semiconductor forms P-type and N-type regions. Based on the characteristics of N-type and P-type semiconductors, it is known that a concentration difference of electrons and holes appears at their junction. Electrons and holes diffuse from the high-concentration region to the low-concentration region, and their diffusion destroys the electrical neutrality at the original junction. PN junction unidirectional conductivity: When a forward voltage V is applied across the PN junction, the equilibrium state of the PN junction is broken under the influence of this external electric field. Holes in the P region and electrons in the N region move towards the PN junction. Holes neutralize the negative ions in the P region of the PN junction, and electrons neutralize the positive ions in the N region of the PN junction, thereby narrowing the PN junction. As the external electric field increases, diffusion motion is further enhanced, and drift motion is weakened. When the external voltage exceeds the threshold voltage, the PN junction acts as a resistor with very low resistance, meaning the PN junction is conducting.
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