Low temperature superconductor and aligned high temperature superconductor magnetic dipole system and method for producing high magnetic fields
A dipole-magnet system and method for producing high-magnetic-fields, including an open-region located in a radially-central-region to allow particle-beam transport and other uses, low-temperature-superconducting-coils comprised of low-temperature-superconducting-wire located in radially-outward-regions to generate high magnetic-fields, high-temperature-superconducting-coils comprised of high-temperature-superconducting-tape located in radially-inward-regions to generate even higher magnetic-fields and to reduce erroneous fields, support-structures to support the coils against large Lorentz-forces, a liquid-helium-system to cool the coils, and electrical-contacts to allow electric-current into and out of the coils. The high-temperature-superconducting-tape may be comprised of bismuth-strontium-calcium-copper-oxide or rare-earth-metal, barium-copper-oxide (ReBCO) where the rare-earth-metal may be yttrium, samarium, neodymium, or gadolinium. Advantageously, alignment of the large-dimension of the rectangular-cross-section or curved-cross-section of the high-temperature-superconducting-tape with the high-magnetic-field minimizes unwanted erroneous magnetic fields. Alignment may be accomplished by proper positioning, tilting the high-temperature-superconducting-coils, forming the high-temperature-superconducting-coils into a curved-cross-section, placing nonconducting wedge-shaped-material between windings, placing nonconducting curved-and-wedge-shaped-material between windings, or by a combination of these techniques.
1. A high-magnetic-field dipole-magnet system comprising:
a plurality of high-temperature-superconducting-coils comprised of windings of high-temperature-superconducting-tape with the width of said high-temperature-superconducting-tape substantially aligned with said high-magnetic-field;
a plurality of low-temperature-superconducting-coils comprised of windings of low-temperature-superconducting-wire;
a cooling system to cool said high-temperature-superconducting-coils and to cool said low-temperature-superconducting-coils;
a first plurality of support-structures located proximate to said high-temperature-superconducting-coils to support said high-temperature-superconducting-coils;
a second plurality of support-structures located proximate to said low-temperature-superconducting-coils to support said low-temperature-superconducting-coils;
a first plurality of electrical-contacts located at the ends of said high-temperature-superconducting-coils to allow electric-current into and out of said high-temperature-superconducting-coils;
a second plurality of electrical-contacts located at the ends of said low-temperature-superconducting-coils to allow electric-current into and out of said low-temperature-superconducting-coils; and
an open-region located in the radially-central-region of said dipole-magnet system.
2. The system in accordance with claim 1 , wherein said high-temperature-superconducting-coils are located in radially-inward-regions of said dipole-magnet.
3. The system in accordance with claim 1 , wherein said low-temperature-superconducting-coils are located in radially-outward-regions of said dipole-magnet.
4. The system in accordance with claim 1 , wherein said high-temperature-superconducting-coils are comprised of bismuth-strontium-calcium-copper-oxide.
5. The system in accordance with claim 1 , wherein said high-temperature-superconducting-coils are comprised of rare-earth-metal, barium-copper-oxide (ReBCO) compounds, wherein said rare-earth-metal is yttrium, samarium, neodymium, or gadolinium or combinations thereof.
6. The system in accordance with claim 1 , wherein said high-temperature-superconducting-tape has a rectangular-cross-section positioned and aligned so that a large-dimension of said rectangular-cross-section is substantially parallel to said high-magnetic-field.
7. The system in accordance with claim 1 , wherein said high-temperature-superconducting-tape has a curved-cross-section comprised of curved-segments separated by a distance positioned and aligned so that said curved-segments of said curved-cross-section are substantially parallel to said high-magnetic-field.
8. The system in accordance with claim 1 , wherein said high-temperature-superconducting-coils are comprised of windings of said high-temperature-superconducting-tape that have a rectangular-cross-section and are positioned and aligned by a nonconducting wedge-shaped-material between said windings of said high-temperature-superconducting-coils so that a large-dimension of said rectangular-cross-section is substantially parallel to said high-magnetic-field.
9. The system in accordance with claim 1 , wherein said high-temperature-superconducting-coils are comprised of windings of said high-temperature-superconducting-tape that have a combination of a rectangular-cross-section and a curved-cross-section, and are positioned and aligned by a nonconducting curved-and-wedge-shaped-material between said windings of said high-temperature-superconducting-coils so that a large-dimension of said rectangular-cross-section and said curved-cross-section is substantially parallel to said high-magnetic-field.
10. A method of producing high-magnetic-fields in a dipole-magnet comprising the steps of:
operating a plurality of high-temperature-superconducting-coils comprised of windings of high-temperature-superconducting-tape with a width of said high-temperature-superconducting-tape substantially aligned with said high-magnetic-field;
operating a plurality of low-temperature-superconducting-coils comprised of windings of low-temperature-superconducting-wire;
operating a cooling system to cool said high-temperature-superconducting-coils and to cool said low-temperature-superconducting-coils;
operating a first plurality of support-structures located proximate to said high-temperature-superconducting-coils to support said high-temperature-superconducting-coils against large Lorentz-forces present in said dipole-magnet;
operating a second plurality of support-structures located proximate to said low-temperature-superconducting-coils to support said low-temperature-superconducting-coils against large Lorentz-forces present in said dipole-magnet;
operating a first plurality of electrical-contacts located at ends of said high-temperature-superconducting-coils to allow electric-current into and out of said high-temperature-superconducting-coils;
operating a second plurality of electrical-contacts located at ends of said low-temperature-superconducting-coils to allow electric-current into and out of said low-temperature-superconducting-coils;
operating an open-region located in a radially-central-region of said dipole-magnet.
11. The method in accordance with claim 10 , wherein said high-temperature-superconducting-coils are located in radially-inward-regions of said dipole-magnet.
12. The method in accordance with claim 10 , wherein said low-temperature-superconducting-coils are located in radially-outward-regions of said dipole-magnet.
13. The method in accordance with claim 10 , wherein said high-temperature-superconducting-coils are comprised of bismuth-strontium-calcium-copper-oxide.
14. The method in accordance with claim 10 , wherein said high-temperature-superconducting-coils are comprised of rare-earth-metal, barium-copper-oxide (ReBCO) compounds, wherein said rare-earth-metal is yttrium, samarium, neodymium, or gadolinium or combinations thereof.
15. The method in accordance with claim 10 , wherein said high-temperature-superconducting-tape has a rectangular-cross-section positioned and aligned so that a large-dimension of said rectangular-cross-section is substantially parallel to said high-magnetic-field.
16. The method in accordance with claim 10 , wherein said high-temperature-superconducting-tape has a curved-cross-section comprised of curved-segments separated by a distance positioned and aligned so that said curved-segments of said curved-cross-section are substantially parallel to said high-magnetic-field.
17. The method in accordance with claim 10 , wherein said high-temperature-superconducting-coils are comprised of windings of said high-temperature-superconducting-tape that have a rectangular-cross-section and are positioned and aligned by nonconducting wedge-shaped-material between said windings of said high-temperature-superconducting-coils so that a large-dimension of said rectangular-cross-section is substantially parallel to said high-magnetic-field.
18. The method in accordance with claim 10 , wherein said high-temperature-superconducting-coils are comprised of windings of said high-temperature-superconducting-tape that have a combination of a rectangular-cross-section and a curved-cross-section, and are positioned and aligned by nonconducting curved-and-wedge-shaped-material between said windings of said high-temperature-superconducting-coils so that a large-dimension of said rectangular-cross-section and said curved-cross-section is substantially parallel to said high-magnetic-field.