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Stackpole RACF Concave Termination Chip Resistor Arrays | NAC Semi

Stackpole RACF Concave Termination Chip Resistor Arrays

Stackpole RACF thick film surface mount resistor arrays use concave terminations and offer isolated or bussed circuits. Compare type code, circuit, resistance, tolerance, power per element, and TCR below. The manufacturer datasheet lists a December 1, 2020 last-time-buy date and recommends RAVF convex arrays as a replacement; verify suitability and availability for your application.

Stackpole RACF series resistors
Representative series image; actual appearance varies by part.

Download the RACF series datasheet (PDF)

Search an exact part number or use the dropdowns to compare characteristics. Select a part number to search NAC Semi.

189 Stackpole RACF parts
Part NumberType CodeCircuitResistanceTolerance (±%)Power per Element at 70 °C (W)TCR (±ppm/°C)Datasheet
Part NumberType CodeCircuitResistanceTolerance (±%)Power per Element at 70 °C (W)TCR (±ppm/°C)Datasheet
RACF102DJT10R0102DIsolated10 Ω50.063250PDF
RACF104DJT100K104DIsolated100 kΩ50.063200PDF
RACF104DJT100R104DIsolated100 Ω50.063200PDF
RACF104DJT10K0104DIsolated10 kΩ50.063200PDF
RACF104DJT10R0104DIsolated10 Ω50.063200PDF
RACF104DJT120K104DIsolated120 kΩ50.063200PDF
RACF104DJT120R104DIsolated120 Ω50.063200PDF
RACF104DJT12K0104DIsolated12 kΩ50.063200PDF
RACF104DJT12R0104DIsolated12 Ω50.063200PDF
RACF104DJT150R104DIsolated150 Ω50.063200PDF
RACF104DJT15K0104DIsolated15 kΩ50.063200PDF
RACF104DJT15R0104DIsolated15 Ω50.063200PDF
RACF104DJT180R104DIsolated180 Ω50.063200PDF
RACF104DJT18K0104DIsolated18 kΩ50.063200PDF
RACF104DJT18R0104DIsolated18 Ω50.063200PDF
RACF104DJT220R104DIsolated220 Ω50.063200PDF
RACF104DJT22K0104DIsolated22 kΩ50.063200PDF
RACF104DJT22R0104DIsolated22 Ω50.063200PDF
RACF104DJT270R104DIsolated270 Ω50.063200PDF
RACF104DJT27K0104DIsolated27 kΩ50.063200PDF
RACF104DJT27R0104DIsolated27 Ω50.063200PDF
RACF104DJT330R104DIsolated330 Ω50.063200PDF
RACF104DJT33K0104DIsolated33 kΩ50.063200PDF
RACF104DJT33R0104DIsolated33 Ω50.063200PDF
RACF104DJT390R104DIsolated390 Ω50.063200PDF
RACF104DJT39K0104DIsolated39 kΩ50.063200PDF
RACF104DJT39R0104DIsolated39 Ω50.063200PDF
RACF104DJT470R104DIsolated470 Ω50.063200PDF
RACF104DJT47K0104DIsolated47 kΩ50.063200PDF
RACF104DJT47R0104DIsolated47 Ω50.063200PDF
RACF104DJT560R104DIsolated560 Ω50.063200PDF
RACF104DJT56K0104DIsolated56 kΩ50.063200PDF
RACF104DJT56R0104DIsolated56 Ω50.063200PDF
RACF104DJT680R104DIsolated680 Ω50.063200PDF
RACF104DJT68K0104DIsolated68 kΩ50.063200PDF
RACF104DJT68R0104DIsolated68 Ω50.063200PDF
RACF104DJT820R104DIsolated820 Ω50.063200PDF
RACF104DJT82K0104DIsolated82 kΩ50.063200PDF
RACF104DJT82R0104DIsolated82 Ω50.063200PDF
RACF164DFT100K164DIsolated100 kΩ10.063200PDF
RACF164DFT10K0164DIsolated10 kΩ10.063200PDF
RACF164DFT11K0164DIsolated11 kΩ10.063200PDF
RACF164DFT15K0164DIsolated15 kΩ10.063200PDF
RACF164DFT1K00164DIsolated1 kΩ10.063200PDF
RACF164DFT2K00164DIsolated2 kΩ10.063200PDF
RACF164DFT470K164DIsolated470 kΩ10.063200PDF
RACF164DFT64K9164DIsolated64.9 kΩ10.063200PDF
RACF164DFT75R0164DIsolated75 Ω10.063200PDF
RACF164DGT100K164DIsolated100 kΩ20.063200PDF
RACF164DGT10K0164DIsolated10 kΩ20.063200PDF
RACF164DGT15K0164DIsolated15 kΩ20.063200PDF
RACF164DGT56K0164DIsolated56 kΩ20.063200PDF
RACF164DJT100K164DIsolated100 kΩ50.063200PDF
RACF164DJT100R164DIsolated100 Ω50.063200PDF
RACF164DJT10K0164DIsolated10 kΩ50.063200PDF
RACF164DJT10R0164DIsolated10 Ω50.063200PDF
RACF164DJT110K164DIsolated110 kΩ50.063200PDF
RACF164DJT110R164DIsolated110 Ω50.063200PDF
RACF164DJT11K0164DIsolated11 kΩ50.063200PDF
RACF164DJT11R0164DIsolated11 Ω50.063200PDF
RACF164DJT120K164DIsolated120 kΩ50.063200PDF
RACF164DJT120R164DIsolated120 Ω50.063200PDF
RACF164DJT12K0164DIsolated12 kΩ50.063200PDF
RACF164DJT12R0164DIsolated12 Ω50.063200PDF
RACF164DJT13K0164DIsolated13 kΩ50.063200PDF
RACF164DJT13R0164DIsolated13 Ω50.063200PDF
RACF164DJT150K164DIsolated150 kΩ50.063200PDF
RACF164DJT150R164DIsolated150 Ω50.063200PDF
RACF164DJT15K0164DIsolated15 kΩ50.063200PDF
RACF164DJT15R0164DIsolated15 Ω50.063200PDF
RACF164DJT160R164DIsolated160 Ω50.063200PDF
RACF164DJT16K0164DIsolated16 kΩ50.063200PDF
RACF164DJT16R0164DIsolated16 Ω50.063200PDF
RACF164DJT180K164DIsolated180 kΩ50.063200PDF
RACF164DJT180R164DIsolated180 Ω50.063200PDF
RACF164DJT18K0164DIsolated18 kΩ50.063200PDF
RACF164DJT18R0164DIsolated18 Ω50.063200PDF
RACF164DJT1K00164DIsolated1 kΩ50.063200PDF
RACF164DJT1K10164DIsolated1.1 kΩ50.063200PDF
RACF164DJT1K20164DIsolated1.2 kΩ50.063200PDF
RACF164DJT1K30164DIsolated1.3 kΩ50.063200PDF
RACF164DJT1K50164DIsolated1.5 kΩ50.063200PDF
RACF164DJT1K60164DIsolated1.6 kΩ50.063200PDF
RACF164DJT1K80164DIsolated1.8 kΩ50.063200PDF
RACF164DJT1M00164DIsolated1 MΩ50.063200PDF
RACF164DJT200K164DIsolated200 kΩ50.063200PDF
RACF164DJT200R164DIsolated200 Ω50.063200PDF
RACF164DJT20K0164DIsolated20 kΩ50.063200PDF
RACF164DJT20R0164DIsolated20 Ω50.063200PDF
RACF164DJT220K164DIsolated220 kΩ50.063200PDF
RACF164DJT220R164DIsolated220 Ω50.063200PDF
RACF164DJT22K0164DIsolated22 kΩ50.063200PDF
RACF164DJT22R0164DIsolated22 Ω50.063200PDF
RACF164DJT240R164DIsolated240 Ω50.063200PDF
RACF164DJT24K0164DIsolated24 kΩ50.063200PDF
RACF164DJT24R0164DIsolated24 Ω50.063200PDF
RACF164DJT270R164DIsolated270 Ω50.063200PDF
RACF164DJT27K0164DIsolated27 kΩ50.063200PDF
RACF164DJT27R0164DIsolated27 Ω50.063200PDF
RACF164DJT2K00164DIsolated2 kΩ50.063200PDF
RACF164DJT2K20164DIsolated2.2 kΩ50.063200PDF
RACF164DJT2K40164DIsolated2.4 kΩ50.063200PDF
RACF164DJT2K70164DIsolated2.7 kΩ50.063200PDF
RACF164DJT300K164DIsolated300 kΩ50.063200PDF
RACF164DJT300R164DIsolated300 Ω50.063200PDF
RACF164DJT30K0164DIsolated30 kΩ50.063200PDF
RACF164DJT30R0164DIsolated30 Ω50.063200PDF
RACF164DJT330K164DIsolated330 kΩ50.063200PDF
RACF164DJT330R164DIsolated330 Ω50.063200PDF
RACF164DJT33K0164DIsolated33 kΩ50.063200PDF
RACF164DJT33R0164DIsolated33 Ω50.063200PDF
RACF164DJT360R164DIsolated360 Ω50.063200PDF
RACF164DJT36K0164DIsolated36 kΩ50.063200PDF
RACF164DJT36R0164DIsolated36 Ω50.063200PDF
RACF164DJT390R164DIsolated390 Ω50.063200PDF
RACF164DJT39K0164DIsolated39 kΩ50.063200PDF
RACF164DJT39R0164DIsolated39 Ω50.063200PDF
RACF164DJT3K00164DIsolated3 kΩ50.063200PDF
RACF164DJT3K30164DIsolated3.3 kΩ50.063200PDF
RACF164DJT3K60164DIsolated3.6 kΩ50.063200PDF
RACF164DJT3K90164DIsolated3.9 kΩ50.063200PDF
RACF164DJT430R164DIsolated430 Ω50.063200PDF
RACF164DJT43K0164DIsolated43 kΩ50.063200PDF
RACF164DJT43R0164DIsolated43 Ω50.063200PDF
RACF164DJT470K164DIsolated470 kΩ50.063200PDF
RACF164DJT470R164DIsolated470 Ω50.063200PDF
RACF164DJT47K0164DIsolated47 kΩ50.063200PDF
RACF164DJT47R0164DIsolated47 Ω50.063200PDF
RACF164DJT4K70164DIsolated4.7 kΩ50.063200PDF
RACF164DJT510K164DIsolated510 kΩ50.063200PDF
RACF164DJT510R164DIsolated510 Ω50.063200PDF
RACF164DJT51K0164DIsolated51 kΩ50.063200PDF
RACF164DJT51R0164DIsolated51 Ω50.063200PDF
RACF164DJT56R0164DIsolated56 Ω50.063200PDF
RACF164DJT5K10164DIsolated5.1 kΩ50.063200PDF
RACF164DJT5K60164DIsolated5.6 kΩ50.063200PDF
RACF164DJT620K164DIsolated620 kΩ50.063200PDF
RACF164DJT620R164DIsolated620 Ω50.063200PDF
RACF164DJT62K0164DIsolated62 kΩ50.063200PDF
RACF164DJT680R164DIsolated680 Ω50.063200PDF
RACF164DJT68K0164DIsolated68 kΩ50.063200PDF
RACF164DJT68R0164DIsolated68 Ω50.063200PDF
RACF164DJT6K20164DIsolated6.2 kΩ50.063200PDF
RACF164DJT750K164DIsolated750 kΩ50.063200PDF
RACF164DJT750R164DIsolated750 Ω50.063200PDF
RACF164DJT75K0164DIsolated75 kΩ50.063200PDF
RACF164DJT75R0164DIsolated75 Ω50.063200PDF
RACF164DJT7K50164DIsolated7.5 kΩ50.063200PDF
RACF164DJT820R164DIsolated820 Ω50.063200PDF
RACF164DJT82K0164DIsolated82 kΩ50.063200PDF
RACF164DJT82R0164DIsolated82 Ω50.063200PDF
RACF164DJT8K20164DIsolated8.2 kΩ50.063200PDF
RACF164DJT910R164DIsolated910 Ω50.063200PDF
RACF164DJT91K0164DIsolated91 kΩ50.063200PDF
RACF164DJT91R0164DIsolated91 Ω50.063200PDF
RACF164DJT9K10164DIsolated9.1 kΩ50.063200PDF
RACF164DZT0R00164DIsolated0 ΩPDF
RACF324DFT1K00324DIsolated1 kΩ10.125200PDF
RACF324DJT100K324DIsolated100 kΩ50.125200PDF
RACF324DJT100R324DIsolated100 Ω50.125200PDF
RACF324DJT10K0324DIsolated10 kΩ50.125200PDF
RACF324DJT12K0324DIsolated12 kΩ50.125200PDF
RACF324DJT150R324DIsolated150 Ω50.125200PDF
RACF324DJT1K00324DIsolated1 kΩ50.125200PDF
RACF324DJT1K50324DIsolated1.5 kΩ50.125200PDF
RACF324DJT220R324DIsolated220 Ω50.125200PDF
RACF324DJT22K0324DIsolated22 kΩ50.125200PDF
RACF324DJT22R0324DIsolated22 Ω50.125200PDF
RACF324DJT2K00324DIsolated2 kΩ50.125200PDF
RACF324DJT2K20324DIsolated2.2 kΩ50.125200PDF
RACF324DJT330R324DIsolated330 Ω50.125200PDF
RACF324DJT33K0324DIsolated33 kΩ50.125200PDF
RACF324DJT47K0324DIsolated47 kΩ50.125200PDF
RACF324DJT4K70324DIsolated4.7 kΩ50.125200PDF
RACF324DJT51R0324DIsolated51 Ω50.125200PDF
RACF324DJT560R324DIsolated560 Ω50.125200PDF
RACF324DJT820R324DIsolated820 Ω50.125200PDF
RACF324DZT0R00324DIsolated0 ΩPDF
RACF408MJT470R408MBussed470 Ω50.063200PDF
RACF648NJT10K0648NBussed10 kΩ50.063200PDF
RACF648NJT3K30648NBussed3.3 kΩ50.063200PDF
RACF648NJT470R648NBussed470 Ω50.063200PDF
RACF648RJT100R648RBussed100 Ω50.063200PDF
RACF648RJT10K0648RBussed10 kΩ50.063200PDF
RACF648RJT150K648RBussed150 kΩ50.063200PDF
RACF648RJT1K00648RBussed1 kΩ50.063200PDF
RACF648RJT22K0648RBussed22 kΩ50.063200PDF
RACF648RJT2K20648RBussed2.2 kΩ50.063200PDF
RACF648RJT4K70648RBussed4.7 kΩ50.063200PDF

Power is rated per element at 70 °C. Zero-ohm jumper entries have no inferred power, tolerance, or TCR. Consult the datasheet for circuit diagrams, voltage limits, and derating.