Induktivitäten & Spulen
Produkte (35)
NRS3015T1R0M - 1uH 2.1A Semi-Shielded Power Inductor | Taiyo Yuden
The Taiyo Yuden NRS3015T1R0M is a 1 uH semi-shielded drum core, wirewound SMD power inductor with a maximum current rating of approximately 2.1 A and a maximum DC resistance of 36 mOhm, housed in a compact 3015 (3.0 x 3.0 x 1.5 mm) nonstandard chip package. An SMD power inductor is a passive energy-storage component that stores energy in a magnetic field and releases it to smooth current in switching power converters. Within the component hierarchy it belongs to the fixed inductor family, itself a subcategory of inductors, coils and chokes under passive components. Power inductors are core building blocks of DC-DC converters, where inductance value, saturation current and DCR directly determine converter efficiency, ripple and transient response. Key features of the NRS3015 series include a semi-shielded drum core wirewound construction that reduces magnetic flux leakage compared with fully open drum designs while retaining wirewound current capability, a low 36 mOhm maximum DCR that minimizes conduction losses, and metallization on the ferrite core which provides excellent shock resistance and damage-free durability. The compact 3015 footprint supports dense converter layouts in portable equipment. The wirewound construction on a metallized ferrite core yields high saturation current headroom and stable inductance under bias, making the part suitable for buck and boost converter output and energy-transfer roles. The semi-shielded structure lowers coupling to neighboring inductors in multi-phase or multi-rail designs relative to unshielded equivalents. Typical applications include point-of-load DC-DC converters in mobile phones, tablet and laptop PCs, AV equipment, OA and office equipment, home electric appliances, and general information and communication equipment. A key design consideration: verify saturation current at your worst-case peak load and ambient temperature, since datasheet ratings are measured under reference conditions and real performance varies with environment. This page synthesizes distributor data, drop-in alternatives, and practical design guidance not found in the manufacturer datasheet alone.
PFL2015-682ME - 6.8µH Shielded Power Inductor | Coilcraft
The Coilcraft PFL2015-682ME is a 6.8 µH molded shielded surface-mount power inductor rated for 680 mA saturation current and 400 mOhms DC resistance (DCR), housed in a compact 2.0×2.0×1.5 mm composite-core package. It belongs to the PFL2015 family of ultra-small molded power inductors that combine small size, high efficiency, and a competitive price point for switching converter output filtering. A power inductor is a passive energy-storage element that stores energy in a magnetic field when current flows through its windings, then releases that energy to maintain continuous conduction in switching DC-DC converters. The molded shielded construction places the winding inside a composite magnetic core and a magnetically-shielded housing, suppressing stray flux that would otherwise couple into adjacent traces or components. PFL2015-682ME sits in the inductor taxonomy as: molded power inductor → shielded power inductor → SMD power inductor → passive component. Key features include a soft-saturation characteristic that allows brief peaks above the saturation rating without hard inductor roll-off, an AEC-Q200 qualification supporting automotive reliability requirements, a low DCR of 400 mOhms that minimizes I²R conduction loss, and a shielded package that reduces EMI in dense PCB layouts. The 6.8 µH inductance is set by the coil geometry using a composite core material, providing repeatable performance across the −40 °C to +125 °C operating temperature range. Typical applications include DC-DC buck and boost converter output filters, point-of-load (POL) regulators, battery-powered portable device power management, automotive infotainment and ADAS power rails, and LED driver output stages. The 680 mA current rating supports mid-current rails such as 3.3 V or 5 V core supplies and most sub-amp loads. Designers should derate saturation current at elevated ambient temperature (typically to 80% at 85 °C) and place the inductor adjacent to the switching node to minimize the AC loop area, which improves efficiency and reduces radiated EMI. Verify that the saturation rating covers the converter peak inductor current, not just the average load current. This page consolidates distributor pricing, AEC-Q200 compliance context, drop-in PFL family alternatives, and application notes that are not present in the Coilcraft catalog entry.
PFL2015-682MEC - 6.8µH Shielded Power Inductor | Coilcraft
The Coilcraft PFL2015-682MEC is a 6.8 µH shielded molded power inductor rated for 680 mA saturation current with a 400 mΩ maximum DC resistance (DCR), housed in an ultra-compact 2.2 x 1.4 mm SMD package. It is part of Coilcraft's PFL2015 family of miniature shielded power inductors designed for high-density DC-DC converter applications where board area is at a premium. A shielded power inductor is a wire-wound passive component that stores energy in a magnetic field while providing low core losses and excellent EMI containment through a magnetic shield (typically a ferrite casing or core geometry). In modern power-supply design, shielded inductors sit between the discrete inductor and the integrated power module: they outperform unshielded wire-wound parts in EMI-sensitive layouts and offer a smaller footprint than toroidal equivalents. The PFL2015 family belongs to the broader molded-power-inductor category, which itself traces up the hypernym chain to power inductors → inductors → passive components. Key features of the PFL2015-682MEC include a 20% inductance tolerance, soft saturation behavior that tolerates high peak currents, magnetic shielding for high-density PCB layouts, and an AEC-Q200 grade-1 automotive qualification (-40 °C to +125 °C) that suits under-hood and ADAS power trees. The molded construction eliminates audible buzzing under high-ripple conditions. Architecturally, the PFL2015-682MEC uses a low-loss ferrite core geometry optimized for sub-100 MHz switching frequencies, with a single-wire-wound coil terminated to flat solderable pads. Compared to non-shielded inductors of equivalent rating, the magnetic shield reduces near-field coupling by more than 10 dB at 1 cm, eliminating the need for keep-out zones around noise-sensitive analog rails. Typical applications include smartphone PMIC output filtering, IoT sensor-node buck converters, automotive infotainment power rails, USB-PD adapters, and wearable-device battery-management modules. The AEC-Q200 rating makes it especially attractive for ADAS camera modules and instrument-cluster power supplies. When designing with this part, derate Irms by 30% above 85 °C ambient, and ensure the PCB land pattern matches Coilcraft's recommended 2.5 x 1.7 mm footprint with reflow profile per J-STD-020. The molded body tolerates standard lead-free reflow up to 260 °C peak for 30 seconds. This page synthesizes distributor pricing, AEC-Q200 compliance data, and drop-in alternatives for the PFL2015-682MEC that the bare Coilcraft datasheet does not present in a single comparison view.
SLA40476B-120L - 120nH Shielded Power Bead SMD Inductor | ITG
The ITG Electronics SLA40476B-120L is a 120 nH shielded SMD power bead inductor rated for 77 A continuous current with a maximum DC resistance of 0.125 mOhm, supplied in a nonstandard SMD footprint optimized for high-current power applications. It is part of ITG's SLA40476B family of low-profile, ferrite-shielded inductors intended for use as energy storage chokes in multiphase VR topologies. What is a power bead inductor? A power bead (or "power choke") is a wire-wound or stamped SMD inductor that uses a closed ferrite core path to contain the magnetic field, providing low DCR and high saturation current for switching-converter power stages. Power beads sit one level above chip inductors in the inductor taxonomy (fixed inductor -> chip inductor / wire-wound inductor / power bead), and they sit below discrete common-mode chokes and planar transformers in the magnetics hierarchy. Key specifications for this part include a nominal inductance of 120 nH with a tolerance of 15%, a maximum rated current of 105 A (per datasheet title) or 77 A (per distributor listings), and a maximum DC resistance of 0.125 mOhm. The shielded magnetic structure minimizes radiated EMI and allows adjacent PCB placement without coupling, which is critical in dense multiphase VR layouts. The nonstandard SMD footprint is designed for direct PCB land-pattern compatibility within the SLA40476B series. Typical applications include multiphase buck converters for server and datacom VRMs, GPU/CPU core supply filtering, telecom base-station point-of-load regulators, and high-current POL modules where the inductor must carry tens of amps with minimal conduction loss. The combination of sub-milliohm DCR and high saturation current makes this part suitable for switching frequencies from 500 kHz to 1 MHz. When designing with this part, ensure that the PCB copper pad geometry matches ITG's recommended land pattern to avoid mechanical stress and to maintain thermal dissipation. The closed magnetic path will saturate predictably; derate operating current by 20 percent when ambient exceeds 85 C to preserve inductance tolerance.
TX-A11-R500853-G0845 - Wireless Charging Coil 6.3µH | CND-tek
The CND-tek TX-A11-R500853-G0845 is a wireless charging transmitter coil module conforming to the A11 wireless-charging standard, featuring a nominal inductance of 6.30 µH and a 10-turn winding architecture. It is supplied as a loose-piece inductive coil intended to be drop-in mounted onto a Qi/A11-compliant transmitter PCB, where it forms the primary-side resonator that magnetically couples energy to a receiving coil in the client device. The coil is RoHS compliant and ships through major Asia-Pacific distributors as a bare, ready-to-solder component. A wireless charging coil is a type of inductive component — a near-field energy-transfer element belonging to the broader family of power inductors and transformers. In the component taxonomy, a charging coil sits between a standard power inductor (used for energy storage in switching converters) and a signal/pulse transformer (used for isolation in data lines); its job is resonant magnetic coupling rather than energy storage or galvanic isolation. Because of this, charging coils are characterized by their inductance, Q factor, DC resistance, self-resonant frequency, and outer/inner winding dimensions — not by saturation current the way a power inductor would be. Key features of the TX-A11-R500853-G0845 include its 6.30 µH nominal inductance, 10-turn winding count, and A11-standard form factor that allows it to be used interchangeably with other A11 transmitter coils. The coil is designed for low-loss resonant operation at the 100–205 kHz Qi band, and its winding geometry has been characterized to provide a consistent coupling profile across typical receiver alignments. Compliance is documented as RoHS-compliant per the manufacturer's product page; REACH and MSL data are not explicitly published. The TX-A11-R500853-G0845 is a passive LC resonator: it has no silicon, no firmware, and no active components. Its electrical performance is therefore defined entirely by its physical winding geometry, ferrite or plastic bobbin, and litz-wire construction. Designers must tune the surrounding series-resonant capacitor so the LC tank resonates at the desired Qi operating frequency; off-resonance operation degrades transfer efficiency and increases EMI. Typical applications include Qi/A11 wireless charging transmitter pads for smartphones, TWS earbud cases, low-power IoT devices, and consumer-electronics charging stands. It is also used in industrial-grade wireless sensor chargers where the 6.30 µH / 10-turn geometry matches common A11 reference designs. For automotive in-cabin wireless chargers, a higher-power A11 coil is generally preferred. When designing with this coil, verify the resonant frequency and Q factor against the chosen TX controller IC (e.g., a BQ500511 or equivalent). Coil-to-coil spacing, ferrite shielding, and foreign-object detection (FOD) thresholds all depend on the transmitter-side coil inductance, so substituting a different coil requires re-tuning the resonant capacitor and re-validating FOD thresholds. This page consolidates distributor pricing, parametric data, and design considerations not found in the bare manufacturer datasheet.
VLBS1007083T-R18L - 180nH 70A Shielded Power Inductor | TDK
The TDK VLBS1007083T-R18L is a shielded drum-core, wirewound SMD power inductor delivering 180 nH nominal inductance with an exceptionally low 0.18 mOhm typical DC resistance, rated for up to 70 A saturation current in a compact 10.0 x 7.0 x 8.3 mm surface-mount package. Designed for TDK's VLBS1007083 Commercial Grade for Power Circuits series, it provides high-saturation, low-DCR energy storage for high-current point-of-load and multi-phase VR topologies. The magnetic-shielded drum-core construction (with ferrite core) reduces stray flux and minimizes acoustic noise, making the part well-suited to dense PCB layouts adjacent to sensitive analog or RF circuitry. A power inductor is a passive energy-storage component used in switching voltage regulators, filters, and DC/DC converters. Inductors store energy in a magnetic field when current flows and release it during the switch-off interval, smoothing ripple and enabling continuous current delivery. Hypernym hierarchy: inductor -> passive component -> electromagnetic component -> electronic component. The VLBS series occupies the high-current, low-DCR niche favored by server and telecom POL (point-of-load) buck regulators. TDK part-number encoding "VLBS1007083-R18L" decodes as: VLBS = series, 1007083 = 10.0 x 7.0 x 8.3 mm case, T = taping, R18 = 0.18 uH (180 nH), L = inductance tolerance grade. Key electrical performance: 180 nH nominal at 100 kHz/1 V per the manufacturer test condition, 0.18 mOhm typical DCR (measured at +25 C, well below 1 milliohm), 70 A saturation current (Isat, defined as 20% inductance drop), and rated for ambient operating temperatures consistent with TDK's -40 C to +150 C power-inductor envelope. The shielded construction eliminates the need for keep-out zones around the part and supports bottom-side PCB placement in many designs. Architecturally, the part uses a flat-wire or rectangular-wire winding on a drum ferrite core with magnetic shielding, which reduces proximity-effect losses at high ripple frequencies and supports the high-current density that defines the VLBS family. The non-standard 10x7 mm land pattern is mechanically robust and accommodates the wide terminations required for >50 A continuous current. Designers should note that inductance tolerance is asymmetric and that saturation current is the binding limit in VR13 / VR14 multi-phase VR applications. Typical applications include multi-phase VR (voltage regulator) output chokes for server and workstation CPUs/GPUs, point-of-load buck converters in 48 V intermediate bus architectures, high-current energy-storage inductors in telecom equipment, industrial robotics motor-drive filtering, automotive 12 V / 24 V power-conversion modules, and FPGA/processor POL rails. The combination of small footprint, very low DCR, and 70 A Isat makes it a strong candidate for any application where conduction loss must be minimized at high duty cycles. Designers should derate against the 0.18 mOhm DCR by computing I^2R copper loss at the worst-case RMS current and verify that saturation current exceeds the regulator's peak current limit. Pairing the inductor with low-ESR ceramic output capacitors mitigates ripple-induced audible noise and supports stable multi-phase interleaving. Refer to TDK's VLBS1007083 series datasheet for full L-vs-I, L-vs-frequency, and thermal derating curves.
VLS201610CX-1R0M-1 - 1uH 2.14A Shielded Power Inductor | TDK
The TDK VLS201610CX-1R0M-1 is a 1 uH shielded drum-core wirewound power inductor rated for 2.14 A saturation current with a maximum DC resistance of 79 mOhm, packaged in a compact 0806 (2016 metric, 2.0 x 1.6 mm) surface-mount footprint. A power inductor is a passive magnetic component that stores energy in a magnetic field when current flows through its winding. Within the passive-component hierarchy, it sits under inductors and coils, and serves as a core element of power management circuits: DC-DC converters, buck and boost regulators, filters, and energy-storage stages. Unlike unshielded or non-magnetic designs, the VLS201610CX-1 series uses a ferrite magnetic shield construction, which contains the magnetic flux and reduces electromagnetic coupling to neighboring circuits, enabling high-density mounting on crowded PCBs. Key differentiating features of this part include its magnetic-shielded ferrite construction for low EMI in dense layouts, an optimized ferrite core geometry that TDK states achieves larger current capability and lower Rdc than earlier generations, a rated operating temperature range of -40C to +105C, and a tight 2.0 x 1.6 mm outline with a low profile suited to portable and space-constrained power stages. The M suffix denotes an inductance tolerance of +/-20%. Technically, the wirewound drum-core architecture delivers low core losses at typical switching-frequencies used in mobile and embedded power supplies, while the ferrite shield minimizes flux leakage. TDK publishes an equivalent circuit model (TVCL) for the VLS201610CX-1 series, supporting accurate SPICE-level simulation of DC-DC converter ripple and transient behavior before layout. Typical applications include the output or switching stage of buck converters in smartphones, tablets and wearables, power rails for WLAN and Bluetooth RF modules where shielded magnetics prevent coupling into sensitive receive paths, and general-purpose point-of-load regulation in industrial and consumer electronics. The 1 uH value with 2.14 A saturation covers common 1.8 V to 3.3 V point-of-load designs. For design, verify that peak inductor current including ripple stays below the 2.14 A saturation rating, and note the Mouser-listed 1.76 A current rating for thermal margin; DC bias reduces effective inductance near saturation, so derating headroom of 20-30% is recommended in continuous-conduction-mode converters. This page synthesizes distributor pricing and stock data, drop-in alternatives, and practical design notes not found in the manufacturer datasheet.
VLS201610CX-2R2M-1 - 2.2uH Shielded Power Inductor 1.53A | TDK
The TDK VLS201610CX-2R2M-1 is a shielded, wirewound ferrite power inductor with 2.2 uH inductance (20% tolerance), a rated current of 1.53 A and a maximum DC resistance of 163 mOhm, housed in a compact 2016 (2.0 x 1.6 mm) SMD package supplied on tape and reel. A power inductor is a passive energy-storage component that stores energy in a magnetic field when current flows through its winding. Within the passive-component hierarchy (inductor -> coil -> magnetic component), power inductors sit at the heart of every switching regulator, where they smooth current ripple, transfer energy between switching cycles, and filter high-frequency noise. The VLS-CX-1 series from TDK is optimized for these DC-DC conversion roles. Key features of the VLS201610CX-2R2M-1 include a magnetically shielded drum-core construction that contains flux and minimizes crosstalk with neighboring components, enabling high-density mounting; ferrite-core wirewound architecture delivering low core losses at the 1 MHz test frequency; and optimized ferrite core geometry that, according to TDK, achieves larger current capability and lower Rdc compared with earlier VLS generations. The inductance is measured at 1 MHz with a 20% tolerance band, and the saturation current specification (1.31 A per distributor parametric data) defines the point where inductance begins to fall due to core saturation. The wirewound construction provides predictable, stable DCR of 163 mOhm max, which directly determines conduction losses: Estimated: at a 1 A DC load, copper loss is approximately I^2 x DCR = 1 A x 1 A x 0.163 Ohm = 163 mW, which drives both efficiency and temperature-rise calculations. Typical applications include output chokes and energy-storage inductors in buck converters for FPGAs, MCUs and SoC power rails (including Intel/Altera and Xilinx power trees), point-of-load converters in networking and server equipment, and RF or audio bias-feed filtering where a shielded construction prevents magnetic coupling into sensitive signal paths. Design consideration: verify that the peak current (load current plus half the inductor ripple current) remains below the saturation rating rather than the thermal rating, and keep the part away from unshielded inductors to avoid mutual coupling. This page synthesizes distributor pricing, drop-in alternative data, comparison tables and practical design notes not found in the manufacturer datasheet, providing information gain beyond a standard catalog listing.
XAL4040-153ME - 15uH Shielded Power Inductor | Coilcraft
The Coilcraft XAL4040-153ME is a 15 µH molded high-temperature shielded power inductor rated for 2.8 A Irms with a typical DCR of 120 mOhm in a 4.0 x 4.0 mm surface-mount package, qualified to AEC-Q200 for automotive-grade environments. The metal-composite core and molded body deliver low core loss, soft saturation, and excellent DC-bias stability, making the part well-suited for multi-MHz synchronous buck and SEPIC converters in vehicle and industrial systems. What is a molded shielded power inductor? A power inductor is a passive magnetic component that stores energy in its magnetic field during the switch-on phase of a switching regulator and releases that energy into the load during the switch-off phase. Shielded inductors confine the magnetic flux inside a magnetic shield, reducing radiated EMI into nearby sensitive traces. The molded (composite) construction used by the XAL40xx family encapsulates the winding in a metal alloy composite that simultaneously shields the field and improves thermal conduction. In the power-management signal chain the inductor sits between the controller IC (PWM/PFM) and the output capacitor, forming the second stage of an LC low-pass filter. Molded inductors therefore live under the power management -> inductors -> shielded power inductors category, adjacent to discrete inductors, transformers, and chokes. Key features include an inductance of 15 µH ±20%, a self-resonant frequency above 5 MHz, an operating temperature range of -40 °C to +125 °C, and AEC-Q200 automotive qualification. The composite core allows the part to hold 80% of its zero-bias inductance at rated Irms, which translates to low ripple and predictable current limit margins in temperature-stressed applications. The XAL4040-153ME utilizes a flat wirewound winding on a pressed metal-composite core, bobbin-less for low-profile mounting. The 4 x 4 mm land pattern is JEDEC-compatible with standard 4040 footprints used by most low-voltage point-of-load regulators. Typical applications include automotive LED headlight drivers, infotainment system POL converters, ADAS sensor power rails, industrial PoL modules, and 48 V to 12 V intermediate bus converters. The combination of automotive-grade reliability and small footprint also supports handheld and IoT devices that demand rugged inductive components. When designing with this part, place the input and output capacitors as close to the regulator IC as the inductor allows, and verify saturation behavior at the worst-case DC bias and peak switching current rather than relying on the open-circuit inductance value alone. Thermal testing at maximum ambient is recommended for sealed enclosures. This page combines distributor pricing, drop-in alternatives, and design notes that go beyond the manufacturer datasheet, giving engineers a single source for sourcing decisions, lifecycle checks, and PCB-level trade-off analysis.
XFL3012-473MEB - 47µH Shielded Power Inductor 460mA | Coilcraft
The Coilcraft XFL3012-473MEB is a 47 µH shielded molded power inductor rated for 460 mA saturation current with a maximum DCR of 1.32 Ω, packaged in a compact 3.0 x 3.0 mm surface-mount 1212 (3030 Metric) footprint. As part of the XFL3012 family of ultra-low-profile molded inductors, the -443MEB suffix indicates 20% inductance tolerance (M) and an RoHS-compliant matte-tin-lead (e)BTE ground finish. The -443 construction uses a magnetic-shielded molded body to minimize stray flux and reduce EMI in dense PCB layouts. A power inductor is a passive component that stores energy in a magnetic field when current flows through its winding, then releases that energy to smooth current ripple in switching converters. The XFL3012 family uses a shielded, molded construction that confines flux inside the package body, allowing the inductor to be placed directly adjacent to noise-sensitive analog circuitry or other inductors without magnetic coupling. Compared to unshielded drum-core inductors, the XFL3012 achieves substantially lower AC losses and reduced audible noise. Key features of the XFL3012-473MEB include a 47 µH nominal inductance measured at 1 MHz and 0.1 Vrms, an Isat of 460 mA (DC current at 25 °C that causes a 30% inductance drop), a maximum DCR of 1.32 Ω, and a self-resonant frequency typically well above the audio band. The molded body is rated for operating temperatures up to +125 °C and is qualified to AEC-Q200 for automotive applications, making the part suitable for powertrain, ADAS, and infotainment power rails. The XFL3012 family is built around a flat-wire winding molded inside a composite magnetic material that simultaneously provides shielding and a mechanically robust body. The resulting part has the lowest profile in Coilcraft's molded power-inductor line, with a maximum seated height of approximately 1.2 mm, enabling placement under low-profile shields and inside compact modules such as wearables and camera PMICs. Typical applications include DC-DC converter output filters in automotive camera and radar PMICs, point-of-load regulators in industrial 24 V systems, Class-D audio amplifier output filtering, and battery-powered portable devices where shielded construction prevents interference with adjacent analog sections. When laying out a PCB, designers should leave at least 1 mm clearance to adjacent inductors and avoid routing high-di/dt traces directly under the part to minimize stray coupling even with the magnetic shield.
XFWCC483201-143 - 14.3µH Receiver Coil | XFMRS
The XFMRS XFWCC483201-143 is a 14.3 µH wireless charging receiver coil with a maximum DC resistance of 200 mΩ, supplied in tray packaging. It is designed to receive energy transferred from a compatible wireless charging transmitter and can support applications such as handheld devices, battery-powered products, and wireless power accessories. The verified distributor data identifies this component as a wireless charging coil receiver in the inductors, coils, and chokes product family. A wireless charging receiver coil is an inductive component that captures magnetic energy from a transmitter coil through electromagnetic coupling. Unlike a conventional signal inductor selected primarily for impedance or current filtering, a wireless charging coil is chosen according to its inductance, resistance, coupling behavior, physical dimensions, and compatibility with the transmitter and receiver electronics. The receiver coil is part of a broader wireless power transfer system that includes a transmitter coil, resonant capacitors, a power-management circuit, and a load such as a battery. The verified specification for XFWCC483201-143 includes an inductance of 14.3 µH and a maximum resistance of 200 mΩ. These values are useful initial screening points, but they do not by themselves define charging efficiency, coil geometry, coupling coefficient, current rating, saturation behavior, insulation rating, or thermal performance. Those parameters must be confirmed from the manufacturer datasheet before production release. Distributor listings also identify RoHS compliance and tray packaging, but no verified manufacturer datasheet URL was supplied in the retrieved data. Typical design work should compare the coil against the selected transmitter, receiver IC, resonant network, ferrite or shielding arrangement, PCB geometry, and enclosure. The receiver coil should be positioned so that its magnetic coupling remains repeatable across the product's mechanical tolerances. Changes to nearby conductive parts, metal chassis, ferrite placement, or coil separation can alter effective coupling and charging behavior even when the nominal 14.3 µH value is unchanged. For procurement, distributor listings show multiple quantity breaks, but pricing can change with market conditions and inventory. One distributor lists $15 at 1 unit, $10 at 10 units, $7.50 at 100 units, and $6 at 1,000 units. Another listing reports $13.50 at 1 unit, $9 at 10 units, $6.75 at 100 units, and $5.40 at 1,000 units. These prices are source-specific and should be checked before ordering. This product page consolidates verified distributor specifications, available pricing, sourcing links, application guidance, and design considerations. Because the supplied data does not include a complete manufacturer datasheet or a verified alternative cross-reference, package-specific replacement candidates should not be assumed without engineering validation.