
Allicdata Part #: | RSS3W270RJTB-ND |
Manufacturer Part#: |
RSS3W270RJTB |
Price: | $ 0.03 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 270 OHM 3W 5% AXIAL |
More Detail: | 270 Ohms ±5% 3W Through Hole Resistor Axial Flame ... |
DataSheet: | ![]() |
Quantity: | 1000 |
1000 +: | $ 0.02550 |
Series: | RSS, CGS |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 270 Ohms |
Tolerance: | ±5% |
Power (Watts): | 3W |
Composition: | Metal Oxide Film |
Features: | Flame Proof, High Voltage, Pulse Withstanding, Safety |
Temperature Coefficient: | ±300ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.197" Dia x 0.591" L (5.00mm x 15.00mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
Through Hole Resistors
Through hole resistors are a type of electrical component that are typically used for applications that require a larger package size. Their main purpose is to provide passive resistance in a circuit, primarily for impedance matching. The resistor’s valuable characteristics make them ideal for a variety of applications, as they offer accurate current limiting, voltage limiting, and/or current smoothing functions.
RSS3W270RJTB Application Field and Working Principle
The RSS3W270RJTB is a type of through hole resistor with a three-watt rating. This resistor type is used in a variety of circuit applications and offers superior performance and reliability. Its components consist of a metal film, which is the heat-resistant, non-magnetic capacitor placed in the center of the resistor for efficient heat transfer. Around this is a metal case, which allows the element to be mounted on a surface with designated mounting holes.
The RSS3W270RJTB resistor’s working principle is based on the Ohm’s law, which states that the current is inversely proportional to the resistance. The resistance is determined by the ferrite material used in the resistor and its size. At higher temperatures, the resistance increases, whereas colder temperatures decrease the resistance. When a current is passed through the resistor, the heat generated by the current causes the ferrite material to expand, thus increasing the resistance. The metal case helps dissipate the heat generated by the resistor, enabling the device to remain cool.
The RSS3W270RJTB can be used in a wide variety of applications, including power systems, audio circuits, and communications systems. It can be used as a resistor in series or parallel circuits, as well as for bipolar junction transistor ( BJT ) bias stabilization, control of amplifier gain, voltage-egulator circuit voltage adjustment, and voltage measuring circuits. Additionally, these resistors are often used as a load in multiplexers, buffers, switches, and differential amplifiers. The resistor also provides an excellent low-noise result at high frequencies, making it well-suited for use in radio and television broadcast systems, high-speed communication networks, and audio preamplifiers.
The RSS3W270RJTB is a reliable and accurate through-hole resistor that offers superior performance for a variety of applications. It offers excellent dissipative properties, making it a great choice for circuit designs that require resistance values that are both consistent and accurate. Furthermore, its heat dissipating capabilities make it suitable for use in high-power circuits. When faced with a challenging circuit design, the RSS3W270RJTB resistor is a go-to solution.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
RSS3W390RJTR | TE Connectiv... | 0.05 $ | 1000 | RSS3 390R 5% REELEDThroug... |
RSS3W8K2JTB | TE Connectiv... | 0.03 $ | 1000 | RES 8.20K OHM 3W 5% AXIAL... |
RSS3W15KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 15.0K OHM 3W 5% AXIAL... |
RSS3W1K5JTB | TE Connectiv... | 0.03 $ | 1000 | RES 1.50K OHM 3W 5% AXIAL... |
RSS33K9JTB | TE Connectiv... | 0.03 $ | 1000 | RES 3.90K OHM 3W 5% AXIAL... |
RSS3W22RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 22.0 OHM 3W 5% AXIAL2... |
RSS3W47RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 47.0 OHM 3W 5% AXIAL4... |
RSS3W470RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 470 OHM 3W 5% AXIAL47... |
RSS3W27RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 27.0 OHM 3W 5% AXIAL2... |
RSS3W820RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 820 OHM 3W 5% AXIAL82... |
RSS3W220RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 220 OHM 3W 5% AXIAL22... |
RSS3W12RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 12.0 OHM 3W 5% AXIAL1... |
RSS3W150RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 150 OHM 3W 5% AXIAL15... |
RSS3W3K3JTB | TE Connectiv... | 0.03 $ | 1000 | RES 3.30K OHM 3W 5% AXIAL... |
RSS3W12KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 12.0K OHM 3W 5% AXIAL... |
RSS3W56KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 56.0K OHM 3W 5% AXIAL... |
RSS3W15RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 15.0 OHM 3W 5% AXIAL1... |
RSS3W2K7JTB | TE Connectiv... | 0.03 $ | 1000 | RES 2.70K OHM 3W 5% AXIAL... |
RSS3W39RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 39.0 OHM 3W 5% AXIAL3... |
RSS3W330RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 330 OHM 3W 5% AXIAL33... |
RSS3W1K2JTB | TE Connectiv... | 0.03 $ | 1000 | RES 1.20K OHM 3W 5% AXIAL... |
RSS3W82RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 82.0 OHM 3W 5% AXIAL8... |
RSS3W39KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 39.0K OHM 3W 5% AXIAL... |
RSS3W180RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 180 OHM 3W 5% AXIAL18... |
RSS3W270RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 270 OHM 3W 5% AXIAL27... |
RSS3W10KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 10.0K OHM 3W 5% AXIAL... |
RSS3W47KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 47.0K OHM 3W 5% AXIAL... |
RSS3W22KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 22.0K OHM 3W 5% AXIAL... |
RSS3W2K2JTB | TE Connectiv... | 0.03 $ | 1000 | RES 2.20K OHM 3W 5% AXIAL... |
RSS3W56RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 56.0 OHM 3W 5% AXIAL5... |
RSS3W18KJTB | TE Connectiv... | 0.03 $ | 1000 | RES 18.0K OHM 3W 5% AXIAL... |
RSS3W68RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 68.0 OHM 3W 5% AXIAL6... |
RSS3W10RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 10.0 OHM 3W 5% AXIAL1... |
RSS3W680RJTR | TE Connectiv... | 0.05 $ | 1000 | RES 680 OHM 3W 5% AXIAL68... |
RSS3W680RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 680 OHM 3W 5% AXIAL68... |
RSS3W1K0JTB | TE Connectiv... | 0.03 $ | 1000 | RES 1.00K OHM 3W 5% AXIAL... |
RSS3W18RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 18.0 OHM 3W 5% AXIAL1... |
RSS3W390RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 390 OHM 3W 5% AXIAL39... |
RSS3W5K6JTB | TE Connectiv... | 0.03 $ | 1000 | RES 5.60K OHM 3W 5% AXIAL... |
RSS3W120RJTB | TE Connectiv... | 0.03 $ | 1000 | RES 120 OHM 3W 5% AXIAL12... |
RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...

RES WW 7W 5% TH1.3 Ohms 5% 7W Through Ho...

RES 24.9 OHM 1/4W 1% AXIAL24.9 Ohms 1% 0...

RES 2.8 OHM 3W 0.5% WW AXIAL2.8 Ohms 0.5...

RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...

RES 340 OHM 1W 1% WW AXIAL340 Ohms 1% 1W...
