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Improved cryogenic and cryoplant model #1484

@jonmaddock

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@jonmaddock

In GitLab by @mkovari on Nov 22, 2021, 16:18

The model for the cryogenic cooling power, and the electric power to provide this, is very old, and has a number of deficiencies.

The model is based on D.S. Slack, J.A. Kern, J.R., Miller, Cryogenic system design for a compact tokamak reactor, UCRL-98733, DE89 003176 (1989).

  1. Heat conduction through gravity support is based on these assumptions:
Average thermal conductivity of stainless steel between 300 K and 4.5 K 10 W/(mK)
Stress in gravity support 67 MPa
Length of gravity support 1 m
  1. Black body radiation load
    I don't know what this calculation is based on. In any case, it seems to take account solely the inward-facing (plasma-facing) area of the TF coil legs, neglecting the outward facing surface.

  2. AC losses. This formula doesn’t seem to have anything to do with AC losses in the coils.

  3. The code does not take account of high-temperature superconducting current leads, which will certainly be used.

  4. The PF coils seem to have been omitted, both for radiation and for current leads.

  5. We need to allow the TF and PF coils to be at different temperatures. (See also Context in output #1461.)

  6. The hard-coded figure of 13% of the ideal Carnot efficiency is now being changed, but we need to make this relative efficiency as input, as in Commit message showing as COMMIT_MSG #1430.

  7. See also Supporting Freia: support properly or just document workaround? #1252 (Superconducting busbars) and other cryogenic issues.

Comments @cjwgriesel @pc6783 @cz1743 @jmorris-uk @skahn ?

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