Allicdata Part #: | Y1691V0035VV9L-ND |
Manufacturer Part#: |
Y1691V0035VV9L |
Price: | $ 14.91 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | RES NTWRK 2 RES MULT OHM RADIAL |
More Detail: | 13.6k, 6.8k Ohm ±0.005% 100mW Power Per Element Vo... |
DataSheet: | Y1691V0035VV9L Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 13.54860 |
Number of Pins: | 3 |
Height - Seated (Max): | 0.330" (8.38mm) |
Size / Dimension: | 0.295" L x 0.100" W (7.49mm x 2.54mm) |
Supplier Device Package: | -- |
Package / Case: | Radial - 3 Leads |
Mounting Type: | Through Hole |
Applications: | Voltage Divider (TCR Matched) |
Operating Temperature: | -55°C ~ 125°C |
Temperature Coefficient: | ±0.2ppm/°C |
Power Per Element: | 100mW |
Series: | 300144Z |
Resistor-Ratio-Drift: | ±0.1 ppm/°C |
Resistor Matching Ratio: | ±0.005% |
Number of Resistors: | 2 |
Tolerance: | ±0.005% |
Resistance (Ohms): | 13.6k, 6.8k |
Circuit Type: | Voltage Divider |
Part Status: | Active |
Packaging: | Bulk |
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Y1691V0035VV9L is a passive, four-terminal integrated resistive networks with three high precision resistors in a single package. It combines the exceptional performance of high-precision resistors with low-cost functions such as temperature compensation, breakdown voltage protection, and multiple output connections to provide a reliable, cost-effective alternative to discrete components. Y1691V0035VV9L is a resistor network typically used in a wide variety of applications such as signal conditioning, circuit protection, power management, and sensing.
Resistor Network & Arrays
The Y1691V0035VV9L is a passive, four-terminal integrated resistive network with three high-precision resistors in a single package. It combines the exceptional performance of high-precision resistors with low-cost functions such as temperature compensation, breakdown voltage protection, and multiple output connections to provide a reliable, cost-effective alternative to discrete components. Resistor networks are widely used in a variety of applications such as signal conditioning, circuit protection, power management, and sensing.
Resistor networks are typically used to create currents in circuits and to provide adjustable resistances and precise input/output characteristics. They can be connected in series, parallel, and combination circuits to achieve desired values and desired functions. The construction of a resistor network consists of conductive elements such as metallic strips or printed circuit tracks arranged in a group of cells. This layout provides the opportunity to adjust both the current and the voltage in a circuit and helps optimize the levels of voltage and current. Resistors are connected in the network in such a way that the circuit characteristics are determined mainly by the values of the individual components.
Resistor networks are often used in voltage and current division applications where a source has to be divided into precisely defined parts. One example of this is in automotive circuits where precise current flow is required to prevent electric shock. In addition, resistor networks can be used in low-impedance circuits, where a range of precise resistances needs to be provided in order to deliver consistent signals.
Arrays are another type of resistor networks, which consist of a series of individual resistors in a predetermined configuration. Arrays combine the advantages of high-precision resistors with the added benefits of multiple output connections. Most arrays are able to precisely control the currents or voltages applied to various terminals in order to obtain specific output characteristics. Furthermore, arrays are often used to condition low-level voltages and currents as well as providing common-mode feedback attenuation in amplifiers.
Working Principle
Y1691V0035VV9L resistor networks rely upon the principles of Ohm’s law and Kirchoff’s law for operation. Ohm’s law states that “the current flowing in a circuit is equal to the voltage across a circuit divided by the resistance of the circuit”. The voltage across a circuit determines the amount of current flowing in it. In addition, Kirchoff’s current law states that “the sum of the currents entering a node in a circuit is equal to the sum of the currents leaving it”. That is, the total currents coming in and out of a node is conserved.
Y1691V0035VV9L resistor networks are designed to exploit these laws in order to create adjustable resistances and precise input/output characteristics. The resistance of a particular resistor in the network can be altered by changing its resistance value. This allows for the fine-tuning of the output characteristics of the resistor network. Furthermore, the resistors in the network can be adjusted in order to create the desired resistance in the connection between two nodes. By altering the resistance between two nodes, the current flowing in the circuit can be precisely controlled, allowing for the precise regulation of voltages and currents.
Y1691V0035VV9L resistor networks are also often employed in low-impedance circuits to provide precisely regulated signals. Since they are constructed from high-precision resistors, they can provide consistently precise signals. The construction and layout of the resistors in the network ensure the consistent output of the desired signals.
Due to their flexibility and performance, Y1691V0035VV9L resistor networks are becoming increasingly popular amongst electronics designers. Their ability to provide precise control over currents and voltages can be utilized to create robust and reliable circuits. Furthermore, their cost-effectiveness and ease of use make them a valuable asset in any designer’s toolkit.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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Y1692V0607TV9L | Vishay Foil ... | 8.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1691V0009VV0L | Vishay Foil ... | 14.91 $ | 1000 | RES NETWORK 2 RES 20K OHM... |
Y1691V0010VV9L | Vishay Foil ... | 14.91 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1691V0035VV9L | Vishay Foil ... | 14.91 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1691V0055VV9L | Vishay Foil ... | 14.91 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0004BV0L | Vishay Foil ... | 15.26 $ | 1000 | 300190Z 1K/1K B V1k Ohm 0... |
Y1692V0466TT9L | Vishay Foil ... | 16.25 $ | 1000 | 300190ZT 10K/33K T T10k, ... |
Y1691V0169BB9L | Vishay Foil ... | 21.32 $ | 1000 | 300144ZT 1K/13K B B1k, 13... |
Y1691V0410BB9L | Vishay Foil ... | 21.32 $ | 1000 | 300144ZT 12K/1K B B1k, 12... |
Y1691V0523BB9L | Vishay Foil ... | 21.32 $ | 1000 | 300144ZT 1K/15K B B1k, 15... |
Y1691V0689BB9L | Vishay Foil ... | 22.13 $ | 1000 | 300144ZT 17K/20K B B17k, ... |
Y1691V0029BA0L | Vishay Foil ... | 22.74 $ | 1000 | 300144Z 2K/4K B A2k, 4k O... |
Y1691V0387BA9L | Vishay Foil ... | 22.74 $ | 1000 | 300144ZT 6K/14K B A6k, 14... |
Y1691V0001AT9L | Vishay Foil ... | 24.18 $ | 1000 | 300144ZT 10K/10K A T10k O... |
Y1691V0059TT9L | Vishay Foil ... | 24.18 $ | 1000 | 300144ZT 2K/2K T T2k Ohm ... |
Y1691V0167TT9L | Vishay Foil ... | 24.18 $ | 1000 | 300144ZT 5K/8K75 T T5k, 8... |
Y1691V0637TT9L | Vishay Foil ... | 24.18 $ | 1000 | 300144ZT 1K/2K5 T T1k, 2.... |
Y1691V0638TT9L | Vishay Foil ... | 24.18 $ | 1000 | 300144ZT 1K/13K5 T T1k, 1... |
Y1691V0010BA9L | Vishay Foil ... | 24.66 $ | 1000 | 300144ZT 20K/10K B A10k, ... |
Y1691V0058TT9L | Vishay Foil ... | 26.23 $ | 1000 | 300144ZT 2K/20K T T2k, 20... |
Y1691V0660VV9L | Vishay Foil ... | 34.45 $ | 1000 | 300144ZT 10K/6K813 V V6.8... |
Y1692V0004DB9L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES 1K OHM RA... |
Y1692V0094BB0L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0094BB9L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0166BB0L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0230BB0L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0388BB0L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0392BB0L | Vishay Foil ... | 6.29 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y169020R0000F9L | Vishay Foil ... | 18.0 $ | 14 | RES 20 OHM 8W 1% TO220-42... |
Y169025R0000T9L | Vishay Foil ... | 21.38 $ | 84 | RES 25 OHM 8W 0.01% TO220... |
Y1692V0219BB0L | Vishay Foil ... | 6.85 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0024TT0L | Vishay Foil ... | 6.93 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0009VV0L | Vishay Foil ... | 7.36 $ | 1000 | RES NTWRK 2 RES 20K OHM R... |
Y1692V0331TV0L | Vishay Foil ... | 7.36 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0331VV0L | Vishay Foil ... | 7.36 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0347VV0L | Vishay Foil ... | 7.36 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1691V0059BB9L | Vishay Foil ... | 7.39 $ | 1000 | RES NETWORK 2 RES 2K OHM ... |
Y1691V0391BB0L | Vishay Foil ... | 7.39 $ | 1000 | RES NTWRK 2 RES MULT OHM ... |
Y1692V0212BT0L | Vishay Foil ... | 7.77 $ | 1000 | RES NTWRK 2 RES 50K OHM R... |
Y1692V0466TT0L | Vishay Foil ... | 7.77 $ | 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...