
Allicdata Part #: | LT30J-5.0-ND |
Manufacturer Part#: |
LTO030F5R000JTE3 |
Price: | $ 2.65 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | RES 5 OHM 30W 5% TO220 |
More Detail: | 5 Ohms ±5% 30W Through Hole Resistor TO-220-2 Non-... |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | $ 2.65000 |
10 +: | $ 2.57050 |
100 +: | $ 2.51750 |
1000 +: | $ 2.46450 |
10000 +: | $ 2.38500 |
Series: | LTO 30 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 5 Ohms |
Tolerance: | ±5% |
Power (Watts): | 30W |
Composition: | Thick Film |
Features: | Non-Inductive |
Temperature Coefficient: | ±150ppm/°C |
Operating Temperature: | -55°C ~ 150°C |
Package / Case: | TO-220-2 |
Supplier Device Package: | TO-220 |
Size / Dimension: | 0.409" L x 0.126" W (10.40mm x 3.20mm) |
Height - Seated (Max): | 0.650" (16.50mm) |
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 are among the most common components used in many electronic devices. These types of resistors are usually constructed with metal film resistors (MFRs) which are mounted on a board with their leg elements extending through the board. This type of resistors have great advantages over surface mount or chip resistors because they are usually more reliable, easier to install, and usually more durable. They are also more suitable for high voltage applications.
The LTO030F5R000JTE3 is one of the Through Hole Resistors available in the market and it is used for a wide range of application fields. This type of resistors consists of a metal film on a ceramic core substrate with metal leg elements that are extended through holes of the board. It has an operating temperature range of -55 °C to + 175 °C and can handle a maximum current of 5mA. The LTO030F5R000JTE3 has a wide resistance range of 3 ohms to 50 M ohms, making it suitable for different applications.
The LTO030F5R000JTE3 is suitable for applications that require high accuracy and stability in their current or voltage readings. This type of resistor has a tolerance of ±0.05%. It is also suitable for noise reduction in audio and video based circuits. This type of resistor is designed for high speed frequency responses making it suitable for switching applications. It can withstand high frequency signals up to 10 MHz with a minimum power dissipation of 0.3 Watts.
The working principle of thisThrough Hole Resistors is relatively simple. It works by dissipating electrical energy in the form of heat. The resistor\'s resistance value is based on the length and thickness of the resistive material used in the resistor. When a current is passed through the component, a small amount of power is converted to heat and released from the resistor. This heat is the basis of the resistor\'s operation. The higher the current, the higher the heat generated and dissipated.
In addition to its excellent electrical and temperature characteristics, the LTO030F5R000JTE3 also has a very low thermal drift, which means that it does not suffer any significant changes in its resistance value as the temperature changes. This makes it suitable for applications that require accuracy and consistency. This type of resistor also has low parasitic capacitance and inductance allowing for better stability in sensitive circuits.
Overall, the LTO030F5R000JTE3 is one of the most reliable and cost-efficient Through Hole Resistors available in the market. It has impressive electrical and temperature characteristics which makes it suitable for various high-temperature and high accuracy applications. With its wide range of resistances and tolerance, it can effectively reduce noise in audio and video based circuits. It also has a low thermal drift which contributes to its stability and accuracy. This type of resistor is highly reliable and is capable of withstanding high temperatures and high voltage applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LTO030F47R00JTE3 | Vishay Sfern... | 3.38 $ | 154 | RES 47 OHM 30W 5% TO22047... |
LTO050F10R00JTE3 | Vishay Sfern... | -- | 4709 | RES 10 OHM 50W 5% TO22010... |
LTO030F15R00JTE3 | Vishay Sfern... | 3.38 $ | 766 | RES 15 OHM 30W 5% TO22015... |
LTO030F10001JTE3 | Vishay Sfern... | -- | 83 | RES 10K OHM 30W 5% TO2201... |
LTO050FR0100JTE3 | Vishay Sfern... | 5.48 $ | 172 | RES 0.01 OHM 50W 5% TO220... |
LTO030FR0100FTE3 | Vishay Sfern... | 6.19 $ | 226 | RES 0.01 OHM 30W 1% TO220... |
LTO050F1R000JTE3 | Vishay Sfern... | 3.81 $ | 3 | RES 1 OHM 50W 5% TO2201 O... |
LTO030F10000JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 1K OHM 30W 5% TO2201 ... |
LTO030FR0150JTE3 | Vishay Sfern... | 4.5 $ | 157 | RES 0.015 OHM 30W 5% TO22... |
LTO050F10000JTE3 | Vishay Sfern... | 3.81 $ | 1381 | RES 1K OHM 50W 5% TO2201 ... |
LTO050FR0100FTE3 | Vishay Sfern... | 7.53 $ | 194 | RES 0.01 OHM 50W 1% TO220... |
LTO030FR0100JTE3 | Vishay Sfern... | -- | 111 | RES 0.01 OHM 30W 5% TO220... |
LTO030FR0470JTE3 | Vishay Sfern... | -- | 99 | RES 0.047 OHM 30W 5% TO22... |
LTO030FR4700JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 0.47 OHM 30W 5% TO220... |
LTO050FR1000FTE3 | Vishay Sfern... | 6.28 $ | 488 | RES 0.1 OHM 50W 1% TO2201... |
LTO050F2R200FTE3 | Vishay Sfern... | 5.71 $ | 268 | RES 2.2 OHM 50W 1% TO2202... |
LTO050F4R700JTE3 | Vishay Sfern... | 3.81 $ | 1609 | RES 4.7 OHM 50W 5% TO2204... |
LTO050F100R0FTE3 | Vishay Sfern... | 5.71 $ | 66 | RES 100 OHM 50W 1% TO2201... |
LTO030F2R200JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 2.2 OHM 30W 5% TO2202... |
LTO030F10R00JTE3 | Vishay Sfern... | 3.38 $ | 118 | RES 10 OHM 30W 5% TO22010... |
LTO030F5R000JTE3 | Vishay Sfern... | -- | 1000 | RES 5 OHM 30W 5% TO2205 O... |
LTO030F100R0JTE3 | Vishay Sfern... | 3.38 $ | 96 | RES 100 OHM 30W 5% TO2201... |
LTO030FR1000JTE3 | Vishay Sfern... | 3.75 $ | 104 | RES 0.1 OHM 30W 5% TO2201... |
LTO050FR0680JTE3 | Vishay Sfern... | -- | 47 | RES 0.068 OHM 50W 5% TO22... |
LTO030F4R700JTE3 | Vishay Sfern... | 3.38 $ | 102 | RES 4.7 OHM 30W 5% TO2204... |
LTO050F5R000JTE3 | Vishay Sfern... | 4.19 $ | 468 | RES 5 OHM 50W 5% TO2205 O... |
LTO050F10001JTE3 | Vishay Sfern... | 3.81 $ | 520 | RES 10K OHM 50W 5% TO2201... |
LTO050F2R200JTE3 | Vishay Sfern... | 3.81 $ | 1521 | RES 2.2 OHM 50W 5% TO2202... |
LTO030F1R000JTE3 | Vishay Sfern... | -- | 1 | RES 1 OHM 30W 5% TO2201 O... |
LTO050F22R00JTE3 | Vishay Sfern... | 3.81 $ | 1985 | RES 22 OHM 50W 5% TO22022... |
LTO030F22R00JTE3 | Vishay Sfern... | 3.38 $ | 137 | RES 22 OHM 30W 5% TO22022... |
LTO050F100R0JTE3 | Vishay Sfern... | 3.81 $ | 2637 | RES 100 OHM 50W 5% TO2201... |
LTO050FR4700JTE3 | Vishay Sfern... | 3.81 $ | 199 | RES 0.47 OHM 50W 5% TO220... |
LTO030FR0500JTE3 | Vishay Sfern... | 4.12 $ | 46 | RES 0.05 OHM 30W 5% TO220... |
LTO050F47R00JTE3 | Vishay Sfern... | 3.81 $ | 286 | RES 47 OHM 50W 5% TO22047... |
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