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QuickTime™ and a None decompressor are needed to see this picture. CXC EPHIN Status and Alternatives Michael Juda

EPHIN Status and Alternatives

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EPHIN Status and Alternatives. Michael Juda. Outline. EPHIN description Thermal issues +27V rail anomaly and impacts Operations constraints Contingencies Future plans. EPHIN Description. - PowerPoint PPT Presentation

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Page 1: EPHIN Status and Alternatives

QuickTime™ and aNone decompressor

are needed to see this picture. CXC

EPHIN Status and Alternatives

Michael Juda

Page 2: EPHIN Status and Alternatives

EPHIN Status Page 2

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1. EPHIN description2. Thermal issues3. +27V rail anomaly and

impacts4. Operations constraints5. Contingencies6. Future plans

Page 3: EPHIN Status and Alternatives

EPHIN Status Page 3

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are needed to see this picture. CXCEPHIN Description

• EPHIN (Electron, Proton, and Helium Instrument) provides on-board particle radiation sensor for safing function– Flight-spare of EPHIN unit in COSTEP on SOHO

– Contains 7 detectors• Passivated ion-implanted Si (detectors A, B, and F)

• Lithium-drifted Si (detectors C, D, and E)• Scintillator with PMT readout (detector G)

– Signals combined to provide 13 particle “coincidence” channels• 4 electron channels covering 0.25-10.4 MeV• 4 proton channels covering 5-53 MeV• 4 alpha-particle (He) channels covering 5-53 MeV/nucleon

• 1 “Integral” channel for particles with energies higher than the above ranges

Page 4: EPHIN Status and Alternatives

EPHIN Status Page 4

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Page 5: EPHIN Status and Alternatives

EPHIN Status Page 5

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Page 6: EPHIN Status and Alternatives

EPHIN Status Page 6

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• EPHIN data is provided to the on-board computer for potential use in radiation monitoring (RADMON)– Rate data from the 13 coincidence channels– Rate data from the individual detectors (not in RADMON now)

– “Aliveness” data

• The RADMON process currently monitors three of the coincidence channels to identify a high-radiation environment– In high-radiation an on-board sequence is run to safe the science instruments and stop the observing program

Channel Particle Energy Range (MeV) Coincidence ConditionP4GM Protons 5.0 - 8.3 A1 A4 B0 C0 D0 E0 F0 G0P41GM Protons 41.0 - 53.0 A1 A2 B0 C0 D0 E0 F0 G0E1300 Electrons 2.64 - 6.18 A0 A1 B0 C0 D0 E0 F0 G0Xn indicates a detector threshold levelStrike-thru indicates a "NOT" condition

Page 7: EPHIN Status and Alternatives

EPHIN Status Page 7

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• EPHIN is mounted on the sun-ward side of the spacecraft

• Degradation of passive thermal control surfaces (e.g. MLI) has led to temperatures increasing faster than pre-launch expectations

• High temperatures have caused anomalous EPHIN performance– High detector leakage currents at high temperature exceed design capability of +27V supply leading to a current-limit condition

– Drop in +27V supply output that leads to a drop in detector HV

– Hysteresis in temperature to recover from anomaly

• High temperatures could lead to permanent degradation or failure of EPHIN– Drop in HV may lead to loss of compensation in Si(Li) detectors

– Component/workmanship-related failure

Page 8: EPHIN Status and Alternatives

EPHIN Status Page 8

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Page 9: EPHIN Status and Alternatives

EPHIN Status Page 9

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• Reduced HV on detector G reduces its anticoincidence efficiency– Higher E1300 rate observed which could lead to unnecessary radiation safing and lost science time• No evidence in past events of lowered sensitivity to radiation

• Reduced HV on detectors C, D, and E could lead to permanent degradation in their performance– Si(Li) detectors require sufficient HV bias to maintain compensation• HV level unknown (not available in telemetry)

– Increased noise in detectors is expected to lower the sensitivity in the EPHIN coincidence channels

– No degradation observed to-date that can be attributed to the anomaly events (16 episodes)

Page 10: EPHIN Status and Alternatives

EPHIN Status Page 10

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Page 11: EPHIN Status and Alternatives

EPHIN Status Page 11

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• Avoid episodes of +27V rail anomaly as much as possible– Plan observations such that the attitude profile keeps the predicted EPHIN temperature below the onset temperature with a margin• Margin selected to limit episodes to ~5/year• Limit on duration of observations in the 60-130 deg pitch range– Pitch range of concern grows with time as the degradation of thermal control surfaces continues

• Requires extensive (re)work in the long-term schedule

• Constrained science targets are occasionally expected to trigger the anomaly– Schedule a long-duration, cold attitude to follow the science target to speed recovery from the anomalous condition

– Adjust safing time before radiation zone entry to minimize possibility of safing trigger from higher E1300 level

Page 12: EPHIN Status and Alternatives

EPHIN Status Page 12

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• Change thresholds of monitored EPHIN channels or which EPHIN channels are monitored in response to degraded EPHIN performance

• RADMON process has been modified to read HRC anticoincidence and MCP total rate data– HRC antico shield and MCP trigger rates replaced He coincidence channel rates

– HRC rates only reflect the high-energy end of the EPHIN measurements• OK match to P41GM but dynamic range is more limited

• Less good match to E1300 and none to P4GM

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EPHIN Status Page 13

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• Ceiling on HRC rate is lower than where we would normally safe for high-radiation

• Using HRC for safing could lead to unnecessary safing and lost science time

• Use it when EPHIN cannot deliver high-energy monitoring capability

Page 14: EPHIN Status and Alternatives

EPHIN Status Page 14

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• Raise E1300 threshold to minimize possibility of unnecessary safing during +27V rail anomaly episodes

• Investigate the gains from turning off the detector G HV– Less current draw should raise the temperature of the onset of the +27V rail anomaly

– Thresholds in the RADMON process may require modification

• Investigate modifications to the temperature margin used in scheduling observations– Budget to allow for more anomaly occurrences

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EPHIN Status Page 15

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http://hea-www.harvard.edu/~juda/memos/ephin/index.html

General EPHIN Information

http://hea-www.harvard.edu/~juda/memos/ephin/leakage_current/index.html

EPHIN Leakage Currents

EPHIN +27V-rail Supply Current-Limit Episodeshttp://hea-www.harvard.edu/~juda/memos/ephin/current_limit/index.html

HRC Use in RADMON Processhttp://hea-www.harvard.edu/~juda/memos/FN443_HRC_in_RADMON.pdf