Allicdata Part #: | Y4485V0001AT0R-ND |
Manufacturer Part#: |
Y4485V0001AT0R |
Price: | $ 5.57 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | RES NETWORK 2 RES 10K OHM 1610 |
More Detail: | 10k Ohm ±0.05% 50mW Power Per Element Voltage Divi... |
DataSheet: | Y4485V0001AT0R Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 5.06045 |
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: | ±0.01% |
Number of Resistors: | 2 |
Tolerance: | ±0.05% |
Resistance (Ohms): | 10k |
Circuit Type: | Voltage Divider |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
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Resistor Networks, Arrays
The Y4485V0001AT0R is an integrated resistor network that is used in the design of high frequency applications such as RF amplifiers, signal processors, and power converters. It consists of two matched, high frequency, low-inductance resistive elements (R1 and R2) of 4.8 ohms each, and a pair of matched, low impedance Z resistors (R3 and R4) of 0.5 ohms each. The resistors are coupled to form a bridged-tee network which is very stable, and provides a low impedance path when properly balanced.
Application Fields
The Y4485V0001AT0R is primarily used in cellular base station designs, however, its potential applications can range greatly. This integrated resistor network excels in high frequency RF signal processing applications, such as:
- Pulse and frequency generators
- RF amplifiers
- RF signal detectors
- Analog-to-digital and digital-to-analog converters
- Power converters
- RF channelizers
The Y4485V0001AT0R integrated resistor network also has application potential outside the realm of cellular base station designs. It can be utilized in consumer electronics, medical device technologies, and aerospace technologies as well. Its low profile, wide bandwidth, and high stability make it well suited for use in these applications.
Working Principle
The working principle behind the Y4485V0001AT0R is based on the concept of series and parallel resistor networks. A series network consists of two or more resistors which are connected together in a line. A parallel network is composed of two or more resistors that are connected together at each end. This type of network is used to increase or decrease the overall impedance of a circuit.
In the Y4485V0001AT0R, the two high-frequency, low-inductance resistive elements (R1 and R2) are connected in series to form a series resistor network, while the two low impedance Z resistors (R3 and R4) are connected in parallel to form a parallel resistor network. The two networks are then combined to create a bridged-tee network which is able to provide a low impedance path for high frequency applications. Additionally, the high-frequency resistive elements are matched in order to ensure a high level of stability within the network.
Overall, the Y4485V0001AT0R is an integrated resistor network that is ideal for high frequency RF signal processing applications. Its series/parallel construction makes it stable and reliable, while its low profile and high bandwidth capabilities make it suitable for use in a variety of applications. As such, the Y4485V0001AT0R offers a great solution for designers of high frequency electronic systems.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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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...