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In-time retention evaluation by particle balance analysis on HT-7

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Presentation on theme: "In-time retention evaluation by particle balance analysis on HT-7"— Presentation transcript:

1 In-time retention evaluation by particle balance analysis on HT-7
ASIPP In-time retention evaluation by particle balance analysis on HT-7 Y. YANG*, and HT-7 team Institute of Plasma Physics, Chinese Academy of Sciences 2006

2 Outline Particle balance method for retention evaluation in HT-7
ASIPP In-time retention evaluation by particle balance analysis on HT-7 Outline Particle balance method for retention evaluation in HT-7 System error of retention D inventory in HT-7 inner vacuum vessel Conclusions

3 ASIPP Particle balance equation for retention evaluation
In-time retention evaluation by particle balance analysis on HT-7 Particle balance equation for retention evaluation Wall retention is a critical topic for ITER. The long pulses of HT-7 provide good opportunity for the study. Particle balance equation is utilized for retention evaluation since 2004. Working gases: commonly D2, He for a short period. Conditioning : D2 and He during the experimental ran. Pumping: 4 cryo-pumps and 4 TMP station. Vacuum Diagnostics: Six ion gauges for vacuum vessel; One diaphragm gauge for fueling tank; One QMS RGA analyzer. [i] Y. Yang, 16th PSI conference, Portland, USA, (2004)

4 ASIPP Main error sources of particle balance method
In-time retention evaluation by particle balance analysis on HT-7 Main error sources of particle balance method For Vtank, volume of fueling tank, error could be limited lower than 3% (including that from the Gas Injection System). For Ptank, pressure of tank, error could be limited lower than <7%. Error of Qpuff could be limited lower than 10%. For Pvv, pressure of vacuum vessel, error could be <15% after calibration with pure gases. For S, pumping speed, which is obtained by measuring pumping quantity and pressure evolution, error could be suppressed <20%. Error of Qextract could be limited lower than 35%.

5 ASIPP Other potential errors: Pressure distribution (influence Pvv, S)
In-time retention evaluation by particle balance analysis on HT-7 Other potential errors: Pressure distribution (influence Pvv, S) Gas type (influence Pvv) Response time* (influence Pvv, S, Ptank) * for GIS tens of ms, for pumping 1s, for gauge tens to hundreds of ms. Error of absolute retention evaluation: Retention ratio evaluation with particle balance method could be limited lower than 50% value after careful design of Gas Injection System and regular calibration of gauges on HT-7. It’s extremely difficult to suppress error low than 40% value.

6 ASIPP Take shot 78467 as an example: Qpuff=149*2.3=342Pal.
In-time retention evaluation by particle balance analysis on HT-7 Take shot as an example: Qpuff=149*2.3=342Pal. With 3 TMP, pumping speed=843l/s. From QMS, H2/D2=2:3. Conversion factor of D2 for Pvv measurement=2.4. So, Qextract=110Pal retention=68%±16%

7 ASIPP Main error sources of relative evaluation (I)
In-time retention evaluation by particle balance analysis on HT-7 Main error sources of relative evaluation (I) Pressure distribution depends on pumping & puffing position, basically uniform when without plasma pressure (>1e-3Pa) within 300ms. Effect on Pvv, previously ~10%, 0 with the new multi-port P monitoring system. Effect on S, same as Pvv. Magenta: during discharge; Blue: after discharge. Shot 78800, puff from Loc5, pump from Loc3.

8 ASIPP Main error sources of relative evaluation (II) Gas type
In-time retention evaluation by particle balance analysis on HT-7 Main error sources of relative evaluation (II) Gas type QMS shows for pure D2, P2/P4~3% (right upper plot), similar to P1/P2 (~2%) for pure H2. Thus assume P2,P3,P4 represents H2,HD,D2 respectively, and bearing the same partial pressure sensitivity factor. A typical QMS plot is shown (right lower), illustrating that basically H isotopes occupy more than 95% of the residual gas. Effect on Pvv, ~10%. Response time GIS puffs gas into vacuum vessel in tens of ms and distributes evenly in <300 ms. For long pulses, Qextract happens mainly within a few to 10 seconds after plasma termination. QMS samples every 1s, while gauge responses every tens to hundreds of ms.

9 ASIPP Main error sources of relative evaluation (III)
In-time retention evaluation by particle balance analysis on HT-7 Main error sources of relative evaluation (III) Error of Qpuff could be limited lower than 7% (from DAQ). Error of Qextract could be lower than 10% (from QMS) Thus, retention could be compared relatively with the error of <20%. The evaluation is suited for long pulse discharges, which generate big pressure variation and provide long enough time for Residual Gas Analysis.

10 ASIPP In-time retention evaluation by particle balance analysis on HT-7 In HT-7, effective pumping speed is very low during the discharge. Particle balance shows that about 60% of the fuelled gas is retained relatively permanently inside the chamber. Longer pulse tends to cause higher retention quantity. The majority of the dynamic inventory is released and pumped within a couple of seconds after the pulse termination. Nov28 Dec04 Dec12 Dec14 Dec17 Later 1st Boronization 81338 (70s/2.6E20 /80%) 2nd 83000 (300s/5.9E20 /88%) 83026 (300s/5.8E20 /76%) 3rd boronization 84247 (10s/1.2E20 /46%)

11 ASIPP Inventory comparison by relative evaluation
In-time retention evaluation by particle balance analysis on HT-7 Inventory comparison by relative evaluation Pumping speed effect on D retention: not distinguishable. S.N. SD[l/s] H2/D2 Qpuff [Pal/s] Qextract [Pal/s] retention error 78466 369 2/3 321 110 68% 16% 78467 843 342 103 Disruption effect on D retention: disruption favors less retention. S.N. SD[l/s] H2/D2 retention error 79152 843 1/2 89% 3% 79158 77% 5% 79164 62% 8%

12 ASIPP D inventory in HT-7 inner vacuum vessel
In-time retention evaluation by particle balance analysis on HT-7 D inventory in HT-7 inner vacuum vessel All the gauges in the inner vacuum vessel show that pressure drops soon after the plasma is formed, keeps relatively steady in a very low value, and rises quickly to a very high value before decaying gradually. No position inside the chamber is observed to confine large amount of neutral particles during the discharge. Brown, before discharge; Red, during discharge; Blue, after discharge.

13 ASIPP H inventory in HT-7 inner vacuum vessel
In-time retention evaluation by particle balance analysis on HT-7 H inventory in HT-7 inner vacuum vessel QMS shows that hydrogen in the released gas could be after discharge as high as 50% (even higher after boronization). QMS (He plasma) By courtesy of M. SU Large amount of H release during the discharges. H/(H+D) ratio evolution By courtesy of J. HUANG

14 ASIPP Possible mechanism
In-time retention evaluation by particle balance analysis on HT-7 Possible mechanism D is trapped after being puffed into the chamber. When without plasma, it desorbed relatively easier; while with plasma, it’s trapped more firmly. The isotopic exchange leads to the release of H from the bores in graphite tiles. Effective pumping speed is very low during the discharge. Disruption could cause Twall rise in some areas, and suppress retention.

15 ASIPP In-time retention evaluation by particle balance analysis on HT-7 Conclusion After careful design and calibration, error could be 50% for quantitative evaluation of D retention. For relative evaluation error could be suppressed fewer than 20%, providing a practical tool for retention study. Particle balance shows that about 60% of the fuelled gas is retained relatively permanently. More retention happens in longer pulse. Recycled H ranges from 10% to 80% of the released gas after plasma termination, depending on the wall condition. Pumping speed has negligible effect on D retention. Disruption helps to decrease D retention.


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