meeting with ph dt di @ cern 26 march 2013
Download
Skip this Video
Download Presentation
Meeting with PH-DT-DI @ CERN-26 March 2013

Loading in 2 Seconds...

play fullscreen
1 / 25

Meeting with PH-DT-DI @ CERN-26 March 2013 - PowerPoint PPT Presentation


  • 76 Views
  • Uploaded on

Meeting with PH-DT-DI @ CERN-26 March 2013. P rinciple of protection Scheme of KATRIN Magnets. A. Hervé /UW. 4482- Principle of Protection of Katrin Coils. KATRIN is an experiment at KIT to measure the mass of the electron neutrino. and CPS. CPS.

loader
I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
capcha
Download Presentation

PowerPoint Slideshow about ' Meeting with PH-DT-DI @ CERN-26 March 2013' - tolla


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.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.


- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript
meeting with ph dt di @ cern 26 march 2013
Meeting with PH-DT-DI @ CERN-26 March 2013

Principle of protection Schemeof KATRIN Magnets

A. Hervé/UW

4482-Principle of Protection of Katrin Coils

slide2

KATRIN is an experiment at KITto measure the mass of the electron neutrino

and CPS

CPS

Needs line of small solenoids to guide electrons

apparition of a resistive zone r
Apparition of a resistive zone r

Quenchpropagatesveryquicky and generates a voltage that open the diode.

Then the coildischargessafely on itself.

This system is intrinsically safe

typical self decay in 5 s
Typical self decay in ≠ 5 s

It is safe if the coil by construction can supportthe generated hot spot.One can spread more the energy by triggeringthe quench-heaters of the long quenched coil.

slide13

Two-coil set up

  • Quench of one coil near nominal current is likely to trigger quench of the other coil
slide15

Possible problem

  • If coupling is not sufficient, one can use the quench-heaters to induce quenches of the other coils (but one needs a Quench-Detector).
  • However, at reduced current ( < 2/3rdIc) the quench-heaters are not efficient because the coils are much more stable.
  • This is where is the real risk for the multi-coil systems.
slide16

If second coil does not quench

  • Current of the unquenched coil continues to circulate through the opened diode of the quenched coil for a long time!
first risk is to over heat the connecting wires
First risk is to over heat theconnecting wires

One can show that the temperature of a givenwireat time t, is a directlydependent of:

Called the currentload in MIITS

( In adiabatic conditions!)

second risk is to overheat the cold diode connected to its heat sink
Second risk is to overheat thecold diode connected to its heat-sink

Diodes

( Also considered in adiabatic conditions!)

slide20

Two-coil set up - final

  • The trick is to add a dump resistor to make sure the residual current will disappear in a time safe for the cold wires and the diodes
slide21

LHC quench analysis

  • This protection scheme is the one adopted by the LHC with 154 magnets in series!
slide22

LHC quench protection

  • Simplify powering an protection scheme 1/8 of LHC
slide25

Conclusions

  • Each coil is self protected by its cold diode that allows discharge on itself.
  • Detection of quench stops the power supply, and powers the quench-heaters of the quenched coil to better spread the thermal energy in it.
  • If another coil quenches it is treated in the same way but how many coils quench in cascade is uncertain, as it depends for example of the current level.
  • After some time (≠ 30 seconds) the breaker is opened so that all currents disappear in a time safe for the cold wires and the cold diodes
ad