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Electromagnets
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Select From
GMW Dipole Electromagnets (Cu)
Helmholtz Coil Electromagnets (Cu)
Electromagnet Coils (Cu)
Superconducting Dipole Electromagnets (HTS)
High Field Solenoid Coils (HTS)
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We can provide complete
electromagnet systems including appropriate power
supplies, field polarity reversal, field measurement
instrumentation, computer control software, all
cabling, installation, and system testing. The GMW range includes resistive (copper) coil and high temperature supterconducting (HTS) Electromagnets.
Click on the Model below and then check the "Electromagnet Systems" tab, at the top of the page,
for complete systems, including field measurement,
power supply, and magnet control.
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Specifications |
Application |
Model |
Max. Gap |
Pole Face (max. diam.) |
Max. Field (gap) |
GMW Dipole Electromagnets (Cu) |
These
versatile, variable-field Electromagnets are suitable
for sample magnetization, magnetic separation, precision sensor calibration, Hall effect studies,
magneto-optics, ferromagnetic resonance, B-H curves
and EPR/NMR spectroscopy. The
C-Frame and H-Frame Electromagnets have changeable Pole
Caps, and most have adjustable Pole gaps to
enable optimization of the geometry and field to
a specific application.
All of these Electromagnets have iron Yokes and the Poles increase the maximum magnetic field with a given Coil power. The Yoke also provides self shielding to minimize the external fringe magnetize fields. For high magnetic field ramp makes some of these designs can be offered with laminated Yokes and Poles, see 5403AC as an example.
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Miniature
Electromagnets |
5201 |
Projected
Field Electromagnet. Open access for probes, lasers, and microscopes. |
0.3T
(4mm) |
5301 |
Sensor Test Electromagnet. Suitable for long sensor arrays. |
50mT
(25mm) |
| C-Frame Electromagnets |
3470 |
75mm |
40mm |
1.0T
(10mm) |
5403 |
86mm |
76mm |
1.6T
(20mm) |
| 5403EG |
130mm |
76mm |
0.6T
(60mm) |
| 5403AC |
60mm |
76mm |
1.3T
(25mm) |
5501 |
204mm |
250mm |
0.6T
(204mm) |
| H-Frame Electromagnets |
3472 |
115mm |
100mm |
2.1T
(20mm) |
3473 |
125mm |
150mm |
2.4T
(20mm) |
3474 |
160mm |
250mm |
3.0T
(20mm) |
 5414 |
125mm |
315mm |
2.7T
(50mm) |
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GMW Helmholtz
Coil Electromagnets (Cu) |
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I.D. |
Length |
Max.
Field |
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axis Helmholtz Coil Electromagnets provide a relatively
large volume of high uniformity at low fields for
spectrometry, sensor calibration, or magnetic alignment.
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 5451 |
300mm |
338mm |
50mT |
 5452 |
160mm |
122mm |
3mT |
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GMW Electromagnet
Coils (Cu) |
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A*T |
I.D. |
O.D. |
| Coils
from the standard Dipole Electromagnets are offered
as separate items. These can be used to configure
Solenoids, Helmholtz type coils or special electromagnets. |
Circular
Coils |
| 11801523 |
4750 |
47mm |
165mm |
| 11801524 |
4750 |
47mm |
165mm |
| 11901111 |
17,200 |
93mm |
260mm |
| 11801864 |
32,200 |
115mm |
345mm |
| 11801364 |
32,200 |
166mm |
395mm |
| 11801653 |
50,400 |
306mm |
636mm |
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HTS-110 High Field Superconducting
Dipole Electromagnets (HTS) |
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HTS-110’s range of cryogen-free dipole magnets provide excellent vertical, horizontal, and lateral access in a compact configuration. Models up to 7 tesla, with a range of pole gaps and access apertures. Fast ramping. Self shielded for low external fringe field.
See HTS-110 Superconducting Current Leads. |
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See HTS-110 for products and specifications. |
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HTS-110 High Field Solenoid Coils (HTS) |
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Max Pole Gap |
HTS-110 offers a range of cryogen free Solenoid Coils for optical surface characterization and analysis, With a field range up to 5 Tesla and a uniformity better than 1% over the central volume.
See HTS-110 Superconducting Current Leads.
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See HTS-110 for products and specifications. |
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This page was last updated on
17 September, 2009 |
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