Allicdata Part #: | Y1692V0466TT9L-ND |
Manufacturer Part#: |
Y1692V0466TT9L |
Price: | $ 16.25 |
Product Category: | Resistors |
Manufacturer: | Vishay Foil Resistors (Division of Vishay Precision Group) |
Short Description: | 300190ZT 10K/33K T T |
More Detail: | 10k, 33k Ohm ±0.01% 300mW Power Per Element Voltag... |
DataSheet: | Y1692V0466TT9L Datasheet/PDF |
Quantity: | 1000 |
1 +: | $ 14.77350 |
Number of Pins: | 3 |
Height - Seated (Max): | 0.413" (10.49mm) |
Size / Dimension: | 0.575" L x 0.160" W (14.61mm x 4.06mm) |
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: | 300mW |
Series: | 300191Z |
Resistor-Ratio-Drift: | ±0.1 ppm/°C |
Resistor Matching Ratio: | ±0.01% |
Number of Resistors: | 2 |
Tolerance: | ±0.01% |
Resistance (Ohms): | 10k, 33k |
Circuit Type: | Voltage Divider |
Part Status: | Active |
Packaging: | Bulk |
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Resistor Networks, Arrays, have many applications in the fields of electronics engineering. For example, Y1692V0466TT9L is a four resistor network that has become increasingly popular nowadays, due to its high performance and flexibility. It can be used in both analog and digital systems, which makes it an ideal choice for a variety of applications. This article will explain the application field and working principle of Y1692V0466TT9L.
Y1692V0466TT9L is a four terminal resistor network that can serve as a voltage divider, current source, or an active element. It is designed for applications that require many discrete voltages from a few input supply voltages. It is also suitable for applications which require an active element such as a differential amplifier, as well as for applications in which the current consumption of the network must be kept as low as possible.
As a voltage divider, Y1692V0466TT9L is useful for applications that require the output voltage to be adjustable with a single resistor. It can be used to divide input voltages between two or more resistors, with a single point to adjust the output. This allows the network to create a wide variety of output voltage levels. It is also possible to use Y1692V0466TT9L as a current source, where a single resistor can be used to adjust the current flowing through the network.
Y1692V0466TT9L can also be used as an active element, as it is capable of providing the gain necessary for different types of active amplifiers. It is usually used as a differential amplifier, as the gain provided by the network can be adjusted based on the size of the resistors and the voltage applied to the circuit. The current gain of the differential amplifier can be adjusted by connecting a pair of resistors between the output and the input to the amplifier. As a result, high current gains are possible with the Y1692V0466TT9L.
The working principle of Y1692V0466TT9L is based on the principle of voltage divider. In a typical voltage divider circuit, a resistor is connected between a positive and a negative voltage. The output voltage is equal to the voltage difference between both terminals divided by the total resistance of the resistor. By connecting multiple resistors in series, the output voltage can be varied using a single resistor. In Y1692V0466TT9L, the four resistors are placed in series and the output voltage can be varied using a single resistor.
The application field of Y1692V0466TT9L is quite broad. It has been used for applications such as motor control, voltage regulating, signal conditioning, sound mixing and many other purposes. As it is capable of providing a wide range of gain, it is also suitable for precision applications such as medical and instrumentation systems. Its low power consumption also makes it an ideal choice for battery powered operations.
In conclusion, Y1692V0466TT9L is an increasingly popular four resistor network that offers excellent performance and great flexibility. It can be used as a voltage divider, current source, or an active element which makes it ideal for a wide variety of applications. It is also highly efficient and does not consume a lot of power, making it suitable for battery powered operations. As a result, Y1692V0466TT9L is an excellent choice for a variety of engineering projects.
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...