Allicdata Part #: | Y4485V0082BA9W-ND |
Manufacturer Part#: |
Y4485V0082BA9W |
Price: | $ 4.65 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | RES NETWORK 2 RES MULT OHM 1610 |
More Detail: | 5k, 10k Ohm ±0.1% 50mW Power Per Element Voltage D... |
DataSheet: | Y4485V0082BA9W Datasheet/PDF |
Quantity: | 1000 |
2500 +: | $ 4.22280 |
Number of Pins: | 3 |
Height - Seated (Max): | 0.071" (1.80mm) |
Size / Dimension: | 0.160" L x 0.106" W (4.06mm x 2.69mm) |
Supplier Device Package: | -- |
Package / Case: | 1610 J-Lead (3 Terminals) |
Mounting Type: | Surface Mount |
Applications: | Voltage Divider (TCR Matched) |
Operating Temperature: | -65°C ~ 125°C |
Temperature Coefficient: | ±0.2ppm/°C |
Power Per Element: | 50mW |
Series: | DSMZ |
Resistor-Ratio-Drift: | ±0.1 ppm/°C |
Resistor Matching Ratio: | ±0.05% |
Number of Resistors: | 2 |
Tolerance: | ±0.1% |
Resistance (Ohms): | 5k, 10k |
Circuit Type: | Voltage Divider |
Part Status: | Active |
Packaging: | Tray |
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
Resistor Networks, Arrays are essential passive components used in electronic circuits for dividing and distributing signals evenly. Y4485V0082BA9W is a type of resistor network which is used to provide general purpose structures and features for different electronic circuits.
The Y4485V0082BA9W resistor network is composed of eight resistor components which are connected in three different configurations: binary, decimal, and hexadecimal. The resistors are connected to one another in parallel or series to form a single, larger resistive element, known as a resistor ladder. This ladder is then connected to the input of a voltage or current source, and its output is connected to the application\'s load.
The application field of Y4485V0082BA9W is mainly used in controlling the voltage distribution between various components in a circuit. It is suitable for voltage dividers where the precision across the entire resistor network must be maintained. The Y4485V0082BA9W can also be used to provide common electrical paths for the various input and output circuits in a variety of digital systems.
The working principle of the Y4485V0082BA9W is based on the principle of resistive division. The resistors in each leg of the resistor network are connected in a specific pattern; for example, in a binary ladder, two resistors are connected in series. When an input voltage is applied to the resistor network, the voltages drop across each resistor in the ladder create a voltage division pattern. The distribution of the divided voltage depends upon the value of the each resistor in the ladder, and the resistance of the entire ladder. This specific pattern of voltage division is then applied to the load, supplying the desired voltage to each element on the circuit.
The Y4485V0082BA9W resistor networks offer several advantages over single resistors. Firstly, they minimize the number of parts in a circuit as all the desired resistances are connected to one another in a single component. Secondly, the Y4485V0082BA9W resistor network is able to provide more accurate voltage divisions than what a single resistor would. Finally, the Y4485V0082BA9W is relatively inexpensive, making them an ideal choice for digital systems in which cost is an important factor.
In conclusion, the Y4485V0082BA9W resistor network is a popular passive component for providing accurate voltage and current distributions in electronic circuits. This component is usually composed of eight resistor elements that are connected in three different configurations to form a larger resistive element, and its working principle is based on the principle of resistive division. Furthermore, the Y4485V0082BA9W is suitable for projects where cost is an important factor, as it is relatively inexpensive.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
Y4485V0002QT9R | Vishay Foil ... | 11.53 $ | 283 | RES NETWORK 2 RES 5K OHM ... |
Y4485V0091BA9W | Vishay Foil ... | 5.1 $ | 1000 | RES NETWORK 2 RES 500 OHM... |
Y4485V0071BA9R | Vishay Foil ... | 5.2 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y4485V0103QT0W | Vishay Foil ... | 6.02 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y4485V0408QT9L | Vishay Foil ... | 20.53 $ | 1000 | DSMZ 1K4/1K4 TCR0.2 Q T S... |
Y4485V0003BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 9K/1K TCR0.2 B A S W... |
Y4485V0005BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 5K/10K TCR0.2 B A S ... |
Y4485V0006BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 10K/2K TCR0.2 B A S ... |
Y4485V0060BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 2K5/10K TCR0.2 B A S... |
Y4485V0151BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 3K0/9K0 TCR0.2 B A S... |
Y4485V0151BB9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 3K0/9K0 TCR0.2 B B S... |
Y4485V0296BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 3K/2K TCR0.2 B A S W... |
Y4485V0458BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 2K/1K5 TCR0.2 B A S ... |
Y4485V0614BA9W | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 350R/400R TCR0.2 B A... |
Y4485V0626BA9L | Vishay Foil ... | 15.92 $ | 1000 | DSMZ 650R/250R TCR0.2 B A... |
Y4485V0001FQ9W | Vishay Foil ... | 16.23 $ | 1000 | DSMZ 10K/10K TCR0.2 F Q S... |
Y4485V0077BQ9W | Vishay Foil ... | 16.23 $ | 1000 | DSMZ 500R/100R TCR0.2 B Q... |
Y4485V0086BQ9W | Vishay Foil ... | 16.23 $ | 1000 | DSMZ 200R/100R TCR0.2 B Q... |
Y4485V0640BQ9W | Vishay Foil ... | 16.23 $ | 1000 | DSMZ 250R/250R TCR0.2 B Q... |
Y4485V0004BT9L | Vishay Foil ... | 16.67 $ | 1000 | DSMZ 1K/1K TCR0.2 B T S B... |
Y4485V0687AQ9L | Vishay Foil ... | 17.25 $ | 1000 | DSMZ 5K/2K TCR0.2 A Q S B... |
Y4485V0471BA19W | Vishay Foil ... | 17.37 $ | 1000 | V/N 319951 10K/650R B A S... |
Y4485V0616BA9W | Vishay Foil ... | 17.37 $ | 1000 | DSMZ 8K7/300R TCR0.2 B A ... |
Y4485V0627BA59W | Vishay Foil ... | 17.37 $ | 1000 | V/N 321606 10K5/650R B A ... |
Y4485V0071BT9L | Vishay Foil ... | 17.41 $ | 1000 | DSMZ 10K/1K TCR0.2 B T S ... |
Y4485V0069BT9L | Vishay Foil ... | 18.21 $ | 1000 | DSMZ 10K/500R TCR0.2 B T ... |
Y4485V0650AQ9L | Vishay Foil ... | 18.89 $ | 1000 | DSMZ 10K/769R231 TCR0.2 A... |
Y4485V0151QQ9W | Vishay Foil ... | 19.94 $ | 1000 | DSMZ 3K0/9K0 TCR0.2 Q Q S... |
Y4485V0084QT4W | Vishay Foil ... | 20.53 $ | 1000 | V/N 321550 1K/500R Q T B ... |
Y4485V0615QT9W | Vishay Foil ... | 20.53 $ | 1000 | DSMZ 3K28/1K4 TCR0.2 Q T ... |
Y4485V0073QT9L | Vishay Foil ... | 21.5 $ | 1000 | DSMZ 1K/100R TCR0.2 Q T S... |
Y4485V0052QT9W | Vishay Foil ... | 22.54 $ | 1000 | DSMZ 10K/100R TCR0.2 Q T ... |
Y4485V0004BA0R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 1K0/1K0 TCR0.2 B A B... |
Y4485V0004BA9R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 1K0/1K0 TCR0.2 B A S... |
Y4485V0005BA9R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 5K/10K TCR0.2 B A S ... |
Y4485V0060BA9R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 2K5/10K TCR0.2 B A S... |
Y4485V0614BA9R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 350R/400R TCR0.2 B A... |
Y4485V0626BA9R | Vishay Foil ... | 24.8 $ | 1000 | DSMZ 650R/250R TCR0.2 B A... |
Y4485V0001FQ9R | Vishay Foil ... | 25.09 $ | 1000 | DSMZ 10K/10K TCR0.2 F Q S... |
Y4482V0077QT9R | Vishay Foil ... | 30.08 $ | 1000 | DSMZ 500R/100R TCR0.2 Q T... |
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...