Allicdata Part #: | LR1F33K2-ND |
Manufacturer Part#: |
LR1F33K2 |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 33.2K OHM 0.6W 1% AXIAL |
More Detail: | 33.2 kOhms ±1% 0.6W Through Hole Resistor Axial M... |
DataSheet: | LR1F33K2 Datasheet/PDF |
Quantity: | 1000 |
4000 +: | $ 0.00723 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 33.2 kOhms |
Tolerance: | ±1% |
Power (Watts): | 0.6W |
Composition: | Metal Film |
Features: | -- |
Temperature Coefficient: | ±50ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.091" Dia x 0.244" L (2.30mm x 6.20mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through hole resistors, or ThHRs, are one of the oldest types of passive electronic components in the electronics industry. They are composed of a core material –usually ceramic– and a layer of resistance material over its surface. ThHRs offer a wide variety of constructions, sizes, shapes, tolerance levels, and power ratings.
In recent years, ThHRs have been substituted by surface mount components, due to the superior performance and cost of modern surface mount parts. Even so, through hole components remain as a viable technology in certain applications, specially where higher power density or higher temperature are involved.One of those applications is the LR1F33K2 resistor. This through hole resistor, made with a 1µF ceramic core, offers a tolerance of 33kΩ at a full temperature range of -40°C to +150°C. It presents negligible power coefficient, which allows a large summation of current without significant changes in resistance. In addition, this resistor is rated for a power dissipation of up to 7 W, making it suitable for a number of power applications, ranging from linear regulator circuits to HVAC systems.
The working principle of the LR1F33K2 resistor is based on Ohm\'s Law. This physical law states that "the current through a conductor between two points is directly proportional to the potential difference across the two points". This means that the electrical impedance between two points is proportional to its resistance.
In the LR1F33K2 resistor, the core material acts as an insulator with a relatively low resistance value. When a potential difference is applied to the resistor, the core material\'s resistance increases, which reduces the current flow. This increase in core material\'s resistance is proportional to the potential difference applied to it, which is determined by the rated tolerance of 33KΩ at full temperature range.
The ability of the LR1F33K2 to dissipate large amounts of power without significant changes in resistance is due to its negligible power coefficient. Generally speaking, the power coefficient of a resistor is a key factor in determining its power rating. In this case, the power coefficient of the LR1F33K2 is so low that it can dissipate up to 7 W without significant changes in its electrical resistance.
In conclusion, the LR1F33K2 is a through hole resistor with 33KΩ tolerance and power rating up to 7 W. It has a 1µF ceramic core and negligible power coefficient, allowing it to dissipate large sums of power without significant changes in its resistance. This makes it suitable for a variety of power applications where high power density and high temperatures are involved.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LR1F180R | TE Connectiv... | 0.01 $ | 1000 | RES 180 OHM 0.6W 1% AXIAL... |
LR1F110K | TE Connectiv... | 0.01 $ | 1000 | RES 110K OHM 0.6W 1% AXIA... |
LR1F110R | TE Connectiv... | 0.01 $ | 1000 | RES 110 OHM 0.6W 1% AXIAL... |
LR1F11K | TE Connectiv... | 0.01 $ | 1000 | RES 11.0K OHM 0.6W 1% AXI... |
LR1F11R | TE Connectiv... | 0.01 $ | 1000 | RES 11.0 OHM 0.6W 1% AXIA... |
LR1F120K | TE Connectiv... | 0.01 $ | 1000 | RES 120K OHM 0.6W 1% AXIA... |
LR1F12K | TE Connectiv... | 0.01 $ | 1000 | RES 12.0K OHM 0.6W 1% AXI... |
LR1F12R | TE Connectiv... | 0.01 $ | 1000 | RES 12.0 OHM 0.6W 1% AXIA... |
LR1F130K | TE Connectiv... | 0.01 $ | 1000 | RES 130K OHM 0.6W 1% AXIA... |
LR1F130R | TE Connectiv... | 0.01 $ | 1000 | RES 130 OHM 0.6W 1% AXIAL... |
LR1F13K | TE Connectiv... | 0.01 $ | 1000 | RES 13.0K OHM 0.6W 1% AXI... |
LR1F13R | TE Connectiv... | 0.01 $ | 1000 | RES 13.0 OHM 0.6W 1% AXIA... |
LR1F150K | TE Connectiv... | 0.01 $ | 1000 | RES 150K OHM 0.6W 1% AXIA... |
LR1F15K | TE Connectiv... | 0.01 $ | 1000 | RES 15.0K OHM 0.6W 1% AXI... |
LR1F15R | TE Connectiv... | 0.01 $ | 1000 | RES 15.0 OHM 0.6W 1% AXIA... |
LR1F160K | TE Connectiv... | 0.01 $ | 1000 | RES 160K OHM 0.6W 1% AXIA... |
LR1F160R | TE Connectiv... | 0.01 $ | 1000 | RES 160 OHM 0.6W 1% AXIAL... |
LR1F16K | TE Connectiv... | 0.01 $ | 1000 | RES 16.0K OHM 0.6W 1% AXI... |
LR1F16R | TE Connectiv... | 0.01 $ | 1000 | RES 16.0 OHM 0.6W 1% AXIA... |
LR1F180K | TE Connectiv... | 0.01 $ | 1000 | RES 180K OHM 0.6W 1% AXIA... |
LR1F18K | TE Connectiv... | 0.01 $ | 1000 | RES 18.0K OHM 0.6W 1% AXI... |
LR1F18R | TE Connectiv... | 0.01 $ | 1000 | RES 18.0 OHM 0.6W 1% AXIA... |
LR1F1K1 | TE Connectiv... | 0.01 $ | 1000 | RES 1.10K OHM 0.6W 1% AXI... |
LR1F1K2 | TE Connectiv... | 0.01 $ | 1000 | RES 1.20K OHM 0.6W 1% AXI... |
LR1F1K3 | TE Connectiv... | 0.01 $ | 1000 | RES 1.30K OHM 0.6W 1% AXI... |
LR1F1K6 | TE Connectiv... | 0.01 $ | 1000 | RES 1.60K OHM 0.6W 1% AXI... |
LR1F200K | TE Connectiv... | 0.01 $ | 1000 | RES 200K OHM 0.6W 1% AXIA... |
LR1F200R | TE Connectiv... | 0.01 $ | 1000 | RES 200 OHM 0.6W 1% AXIAL... |
LR1F20R | TE Connectiv... | 0.01 $ | 1000 | RES 20.0 OHM 0.6W 1% AXIA... |
LR1F220K | TE Connectiv... | 0.01 $ | 1000 | RES 220K OHM 0.6W 1% AXIA... |
LR1F220R | TE Connectiv... | 0.01 $ | 1000 | RES 220 OHM 0.6W 1% AXIAL... |
LR1F22R | TE Connectiv... | 0.01 $ | 1000 | RES 22.0 OHM 0.6W 1% AXIA... |
LR1F240K | TE Connectiv... | 0.01 $ | 1000 | RES 240K OHM 0.6W 1% AXIA... |
LR1F24K | TE Connectiv... | 0.01 $ | 1000 | RES 24.0K OHM 0.6W 1% AXI... |
LR1F24R | TE Connectiv... | 0.01 $ | 1000 | RES 24.0 OHM 0.6W 1% AXIA... |
LR1F270K | TE Connectiv... | 0.01 $ | 1000 | RES 270K OHM 0.6W 1% AXIA... |
LR1F27K | TE Connectiv... | 0.01 $ | 1000 | RES 27.0K OHM 0.6W 1% AXI... |
LR1F27R | TE Connectiv... | 0.01 $ | 1000 | RES 27.0 OHM 0.6W 1% AXIA... |
LR1F2K0 | TE Connectiv... | 0.01 $ | 1000 | RES 2.00K OHM 0.6W 1% AXI... |
LR1F2K4 | TE Connectiv... | 0.01 $ | 1000 | RES 2.40K OHM 0.6W 1% AXI... |
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