Allicdata Part #: | Y1485V0642QA9L-ND |
Manufacturer Part#: |
Y1485V0642QA9L |
Price: | $ 18.25 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | DSM 10K/399R86 TCR2 Q A S B |
More Detail: | 399.86, 10k Ohm ±0.02% 50mW Power Per Element Volt... |
DataSheet: | Y1485V0642QA9L Datasheet/PDF |
Quantity: | 1000 |
1 +: | $ 16.58250 |
Number of Pins: | 2 |
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: | ±2ppm/°C |
Power Per Element: | 50mW |
Series: | DSM |
Resistor-Ratio-Drift: | ±0.5 ppm/°C |
Resistor Matching Ratio: | ±0.05% |
Number of Resistors: | 2 |
Tolerance: | ±0.02% |
Resistance (Ohms): | 399.86, 10k |
Circuit Type: | Voltage Divider |
Part Status: | Active |
Packaging: | Bulk |
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Resistor networks have extensive practical applications, including in Y1485V0642QA9L. As its name implies, a resistor network is a group of resistors connected in a specific order or configuration to provide a predetermined electrical path or limit current, serve as a voltage divider, or create a certain value of resistance. The resistors are often connected in series or parallel in order to produce a desired impedance, depending on application. This type of resistors network can be quite complex, but the principles of operation are always the same.
Y1485V0642QA9L is an array consisting of two resistor networks, operating in parallel, with the aim of providing a desired impedance or resistance in circuit operations. The two networks consist of four resistors each, meaning that there are eight resistors in total. The two networks are linked by one, and the resistors are connected in series or parallel, depending on their configuration and purpose. By connecting them in different order, new complex resistor networks can be formed, providing an unlimited range of configurations and applied purposes.
The array of Y1485V0642QA9L is basically a combination of individual resistors connected in various ways to give different characteristics and performance, depending on the aim and desired result. By connecting several resistors in parallel, the resistance value is reduced and the current is increased. This allows the values to be more precisely controlled than if only one resistor was used. Similarly, when resistors are connected in series, the resistance increases and the current decreases. This can be used to close off a system or create an alarm. By combining the two resistor networks of Y1485V0642QA9L in various forms, a range of different impedances and behaviors can be produced, making them a versatile and efficient solution to many applications.
The main working principle of Y1485V0642QA9L can be summed up as follows. When resistors are connected in either series or parallel, the individual resistances are combined in a particular way, resulting in desired attributes in terms of the resistance, impedance, and current produced. By connecting the two networks of Y1485V0642QA9L in certain orders, the most effective combination can be achieved, making it a perfect solution for the application.
Y1485V0642QA9L has found a wide range of applications, particularly in the fields of electronics and telecommunications. For example, these resistor arrays are used in telecommunication systems to divide the transmission power into individual signals; they are also used in the switching and control of current in electronic devices and circuits. In addition, they can be used as buffers, current limiters, and temperature sensors, making them indispensable in industrial and consumer electronics.
In conclusion, Y1485V0642QA9L is a type of resistor network that is specifically designed to meet specific application and performance requirements, offering optimal solutions for industrial and consumer applications. By combining two resistor networks in various combinations, the desired impedance and behaviors can be achieved, thus proving to be an incredibly versatile and efficient solution to a range of tasks.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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Y1485V0080AT9W | Vishay Foil ... | 5.06 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0002BA9W | Vishay Foil ... | 15.07 $ | 1000 | DSM 5K/5K TCR2 B A S W5k ... |
Y1485V0296BA9W | Vishay Foil ... | 15.07 $ | 1000 | DSM 3K/2K TCR2 B A S W2k,... |
Y1485V0458BA9W | Vishay Foil ... | 15.07 $ | 1000 | DSM 2K/1K5 TCR2 B A S W1.... |
Y1485V0617BA9L | Vishay Foil ... | 15.07 $ | 1000 | DSM 3K187/6K813 TCR2 B A ... |
Y1485V0618BA9L | Vishay Foil ... | 15.07 $ | 1000 | DSM 5K9/10K TCR2 B A S B5... |
Y1485V0259AT9L | Vishay Foil ... | 16.13 $ | 1000 | DSM 10K0/4K00 TCR2 A T S ... |
Y1485V0642BA9L | Vishay Foil ... | 16.44 $ | 1000 | DSM 10K/399R86 TCR2 B A S... |
Y1485V0103QT9W | Vishay Foil ... | 17.11 $ | 1000 | DSM 2K/3K TCR2 Q T S W2k,... |
Y1485V0071QT9L | Vishay Foil ... | 17.92 $ | 1000 | DSM 10K/1K TCR2 Q T S B1k... |
Y1485V0642QA9L | Vishay Foil ... | 18.25 $ | 1000 | DSM 10K/399R86 TCR2 Q A S... |
Y1485V0011BA9R | Vishay Foil ... | 22.54 $ | 1000 | DSM 1K/4K TCR2 B A S T1k,... |
Y1485V0056BA9R | Vishay Foil ... | 23.16 $ | 1000 | DSM 1K/9K TCR2 B A S T1k,... |
Y1485V0002BT9R | Vishay Foil ... | 23.2 $ | 1000 | DSM 5K0/5K0 TCR2 B T S T5... |
Y1485V0001AA9R | Vishay Foil ... | 4.48 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0001BQ9W | Vishay Foil ... | 4.49 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0001FA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0005BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0085BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0085BA9W | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0089BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES 200 OHM... |
Y1485V0151BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0157BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES 4 OHM 1... |
Y1485V0246BA0L | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0559BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0560BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0581BA9R | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0581BA9W | Vishay Foil ... | 4.52 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0001BA0L | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0001BA0W | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0001BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 10K OHM... |
Y1485V0004BA0R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 1K OHM ... |
Y1485V0004BA0W | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 1K OHM ... |
Y1485V0004BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 1K OHM ... |
Y1485V00082BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0082BA0W | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0082BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0091BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 500 OHM... |
Y1485V0246BA0W | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES MULT OH... |
Y1485V0257BA9R | Vishay Foil ... | 4.64 $ | 1000 | RES NETWORK 2 RES 2.5K OH... |
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...