Allicdata Part #: | Y4942V0001BB0L-ND |
Manufacturer Part#: |
Y4942V0001BB0L |
Price: | $ 5.47 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | RES NTWRK 2 RES 10K OHM RADIAL |
More Detail: | 10k Ohm ±0.1% 300mW Power Per Element Voltage Divi... |
DataSheet: | Y4942V0001BB0L Datasheet/PDF |
Quantity: | 1000 |
500 +: | $ 4.97443 |
Series: | 300190 |
Packaging: | Bulk |
Part Status: | Active |
Circuit Type: | Voltage Divider |
Resistance (Ohms): | 10k |
Tolerance: | ±0.1% |
Number of Resistors: | 2 |
Resistor Matching Ratio: | -- |
Resistor-Ratio-Drift: | -- |
Number of Pins: | 3 |
Power Per Element: | 300mW |
Temperature Coefficient: | ±2ppm/°C |
Operating Temperature: | -55°C ~ 125°C |
Applications: | Voltage Divider (TCR Matched) |
Mounting Type: | Through Hole |
Package / Case: | Radial - 3 Leads |
Supplier Device Package: | Radial Lead |
Size / Dimension: | 0.575" L x 0.160" W (14.61mm x 4.06mm) |
Height - Seated (Max): | 0.413" (10.49mm) |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
The Y4942V0001BB0L is a type of resistor network or array. Resistor networks and arrays are components which, as their name implies, are composed of a number of individual resistors connected together to form a single, integrated device. They offer several potential advantages over individual resistors, including high input/output isolation, high power dissipation, and the ability to provide distributed termination to digital signals.
A Y4942V0001BB0L device, specifically, is a 100-pin staggered column array with a typical resistance of 2.5 ohms. The device provides both excellent signal and power line isolation between input and output. It is rated to dissipate up to 80 mW of power, with a voltage rating of 80 volts and a current of 2 amps. The device also provides a full 0.1 ohm low profile stabilization resistor between the in/out pins.
In terms of its application field, the Y4942V0001BB0L can be used as an isolator in many signal and power line applications. It is especially well-suited to applications in which high levels of isolation are needed, such as in automotive, industrial, HVAC, and telecommunications systems. Additionally, the device is useful for signal conditioning, EMI/RFI filtering, protection circuits, line impedance stabilization networks, DC/DC converters, and power supplies, among other applications.
To understand its inner workings and the principles of operation, it is important to note that this type of laser diode element is composed of multiple pins arranged in a staggered column array. Each pin is connected to one or more resistors, with one end of each resistor connected to a common point. This connection is typically made at the center of the device. The other end of each resistor is then connected to its respective output pin, allowing for signal input and output.
The resistors in the Y4942V0001BB0L array form a lattice network, in which each resistor is connected to both its own input as well as the next resistor’s output. This forms a network in which each element has resistance, current, and voltage levels that factor into the overall operation of the device. The connections formed by the resistors help resist any stray noise in the signal or power lines, resulting in a cleaner transmission.
In terms of operational principles, the resistors work to reduce the overall resistance of the device. As a result, the current required for a certain voltage level is reduced, and the voltage seen by the source is increased. The result is a device that can provide distributed termination, offer high levels of isolation, and dissipate more power while running at lower currents than would a single resistor.
In short, the Y4942V0001BB0L is an excellent resistor array that is capable of providing distributed termination at high levels of isolation while dissipating significant amounts of power. The device is highly useful in a wide variety of applications, from automotive to industrial to telecommunications, and is an excellent choice for any application in which power dissipation and signal isolation are key requirements.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
Y4944V0587TA9L | Vishay Foil ... | 20.37 $ | 1000 | 300192T 50K/50K/5K7 T AOh... |
Y4942V0001BB0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES 10K OHM R... |
Y4942V0053FF0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES 12K OHM R... |
Y4942V0082BB0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0284DD0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0294FF0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0295FF0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0308FF0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0423BB0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4943V0443BB0L | Vishay Foil ... | 5.47 $ | 1000 | RES NTWRK 2 RES 4 OHM RAD... |
Y4942V0082AA0L | Vishay Foil ... | 5.9 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4943V0370BA0L | Vishay Foil ... | 5.9 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0089QQ9L | Vishay Foil ... | 6.02 $ | 1000 | RES NTWRK 2 RES 200 OHM R... |
Y4942V0120BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0120BB9L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0128BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0128BB9L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0133BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES 39K OHM R... |
Y4942V0133BB9L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES 39K OHM R... |
Y4942V0138BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES 70K OHM R... |
Y4942V0138BB9L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES 70K OHM R... |
Y4942V0139BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0219BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0324BB0L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0324BB9L | Vishay Foil ... | 6.08 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0001FT0L | Vishay Foil ... | 6.15 $ | 1000 | RES NTWRK 2 RES 10K OHM R... |
Y4942V0088FT9L | Vishay Foil ... | 6.15 $ | 1000 | RES NTWRK 2 RES 100 OHM R... |
Y4943V0004TT0L | Vishay Foil ... | 6.15 $ | 1000 | RES NTWRK 2 RES 1K OHM RA... |
Y4942V0011VV0L | Vishay Foil ... | 6.4 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0129VV0L | Vishay Foil ... | 6.4 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0132VV0L | Vishay Foil ... | 6.4 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0134TV0L | Vishay Foil ... | 6.4 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0135TV0L | Vishay Foil ... | 6.4 $ | 1000 | RES NTWRK 2 RES 3.3K OHM ... |
Y4942V0130TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0131TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0136TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES 47K OHM R... |
Y4942V0137TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y4942V0403AT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES 25K OHM R... |
Y4943V0136TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES 47K OHM R... |
Y4943V0209TT0L | Vishay Foil ... | 6.76 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
RES NTWRK 18 RES 47 OHM 36LBGA47 Ohm 1% ...
RES NTWRK 32 RES 56 OHM 36LBGA56 Ohm 1% ...
RES ARRAY 4 RES 39 OHM 120639 Ohm 5% 62....
RES ARRAY 4 RES 43 OHM 080443 Ohm 5% 62....
RES ARRAY 4 RES 120 OHM 0804120 Ohm 5% 6...
RES ARRAY 2 RES 300 OHM 0606300 Ohm 5% 6...