1 / 12

Superconductive magnets in LHC.

Superconductive magnets in LHC. The limits of traditional magnets force physicists to use superconducting magnets in LHC experiments. Special situations. The internal Weiss areas play a keyrole in this. The easier these align along the H-field, the bigger µ of the material

quade
Télécharger la présentation

Superconductive magnets in LHC.

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Superconductive magnets in LHC. The limits of traditional magnets force physicists to use superconducting magnets in LHC experiments

  2. Special situations • The internal Weiss areas play a keyrole in this. The easier these align along the H-field, the bigger µ of the material • If H is very big, the increasing alignement of the Weiss areas slows down, because there are at a certain moment no more magnetic dipoles to align • In practice, B reaches a maximum value of 2T, increasing H does not help. CERN HST2001

  3. Limits • They use concrete to stabilize the form of the ferromagnetic yoke. • For a magnetic field of 0,3 T as in the LEP injection dipole magnet, you need a power of 20 kW per magnet. There are some 500 magnets in LEP, this means a total power for these magnets alone of 10 MW. CERN HST2001

  4. The cooling problem • They need lots of water to cool the magnet. • This is a enormous loss of energy. CERN HST2001

  5. One solution: superconductivity! • The LHC requires bending fields of 8,5T to 9T and even more. The current is 13000A • In and µ is constant, a yoke is necessary to make a strong construction, and to guide the return field. To have strong magnetic fields mainly the current should be increased to very high values. To avoid losses due to Ohm’s law-and the corresponding cooling problem- the wires must be superconductive: a temperature of 1,7 K. CERN HST2001

  6. The coil is now crucial. • Since the surface of the yoke no longer determines the form of the magnetic field anymore, only the form of the coil itself can. • The surface of the coil must lie perfectly horizontal, with a perfect vertical field. • This vertical field must be extremely homogenious. • The wrapping of the coil must be very precize: a tolerance of only a few µm is allowed, with a length of 12 meters. CERN HST2001

  7. The magnetic field • The field must also be very stable:constant electrical current • Both beams must be bent: the current goes through both coils (series) • For a vertical field the wrapping must be sinusoidal CERN HST2001

  8. Look carefully CERN HST2001

  9. More about wires CERN HST2001

  10. Cross section CERN HST2001

  11. CERN HST2001

  12. As a consequence • The helium must flow constantly and cool permanently, taking all the heat away • The circuit should continuously be able to cool all helium to this low temperature • They will need 5000 tons of helium in this giant magnet, the production of the whole world during one year CERN HST2001

More Related