A range of solid and split Ferrite Sleeves, which can be used as suppression cores and shielding beads for round cables. They are available for a wide range of cable diameters.
Split Ferrite Sleeves (or cores) are clamp type sleeve that are used as suppression cores. They feature A5 material cores that are installed around a cable. They are ideal for making estimations in EMI precaution and attenuate any form of EMI emission. The polyamide case simplifies assembly of the core in equipment, where retrofit and testing is a necessity. The high performance magnetic material allows for protection from unwanted EMI radiation , without affecting the wave forms, in digital equipment. They can be used for personal computers, word processors, fax machines, display equipment, photocopiers, and computer consoles. This protection ensures immunity against transmission and other types of noise in such equipment, which is essential. They can be mounted on to both a cable with a connector and a wired harness. They binding band ensures the cable is securely fixed.
Solid Ferrite Sleeves are a broad selection of shielding beads that guarantee impedance specifications over a wide frequency range. This range includes options that are mainly applied to wire assemblies and the MATV CATV industries. The range also includes options with a ring configuration that provides greater utilisation of the ferrite material properties, which can be used for a wide frequency range and are mainly used as multi-turn suppression cores.
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Use the filters or search below to find what you're looking for
| Price range | Availability | Impedance 100 MHz | Overall Length | Impedance 25 MHz | Outside Height | Maximum Compatible Cable Diameter | Overall Width | View | |
|---|---|---|---|---|---|---|---|---|---|
| R 73,3916 - R 81,5461 | Request the lead time here |
214 Ω
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1.299 in
33.0 mm
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141 Ω
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0.819 in
20.8 mm
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0.276 in
7.0 mm
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0.748 in
19.0 mm
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| R 4,0849 - R 4,5388 | Request the lead time here |
73 Ω
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0.551 in
14.0 mm
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45 Ω
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| R 5,1733 - R 5,7481 | Request the lead time here |
138 Ω
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0.63 in
16.0 mm
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87 Ω
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| R 6,0732 - R 6,748 | Request the lead time here |
146 Ω
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0.728 in
18.5 mm
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101 Ω
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| R 8,8411 - R 9,8235 | Request the lead time here |
260 Ω
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1.181 in
30.0 mm
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180 Ω
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| R 4,187 - R 4,6523 | Request the lead time here |
75 Ω
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0.472 in
12.0 mm
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39 Ω
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| R 4,3831 - R 4,8701 | Request the lead time here |
72 Ω
|
0.492 in
12.5 mm
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42 Ω
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| R 11,0381 - R 12,2645 | Request the lead time here |
204 Ω
|
0.925 in
23.5 mm
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127 Ω
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| R 8,0982 - R 8,998 | Request the lead time here |
171 Ω
|
0.748 in
19.0 mm
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107 Ω
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| 10319116 | R 15,5082 - R 17,2314 | Request the lead time here |
258 Ω
|
1.125 in
28.57 mm
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164 Ω
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| R 8,277 - R 9,1967 | Request the lead time here |
163 Ω
|
0.787 in
20.0 mm
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111 Ω
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| R 14,3734 - R 15,9704 | Request the lead time here |
178 Ω
|
1.102 in
28.0 mm
|
104 Ω
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| R 17,9288 - R 19,9208 | Request the lead time here |
242 Ω
|
1.122 in
28.5 mm
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143 Ω
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| R 16,4401 - R 18,2668 | Request the lead time here |
209 Ω
|
1.102 in
28.0 mm
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124 Ω
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| R 14,1758 - R 15,7508 | Request the lead time here |
105 Ω
|
1.142 in
29.0 mm
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60 Ω
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| R 0,4447 - R 0,494 | Request the lead time here |
52 Ω
|
0.157 in
4.0 mm
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33 Ω
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| R 0,6621 - R 0,7357 | Request the lead time here |
51 Ω
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0.157 in
4.0 mm
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32 Ω
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| R 0,4858 - R 0,5398 | Request the lead time here |
55 Ω
|
0.197 in
5.0 mm
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37 Ω
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| R 0,4654 - R 0,5171 | Request the lead time here |
61 Ω
|
0.197 in
5.0 mm
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37 Ω
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| R 0,4866 - R 0,5408 | Request the lead time here |
48 Ω
|
0.197 in
5.0 mm
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27 Ω
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