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Future efforts could faster-burning igniters (pyrogen or BKNO3), higher surface area propellants (pixie dust), or additional mechanical retention. While chuffing represents a minor issue on this flight, successful, rapid, and complete ignition is a necessary technical milestone for multistage flight. Care must still be taken to not over-pressurize the case or clog the nozzle with a large igniter.
Recovery
Piston Deployment
Firing Force
Comparison with Ground Test
Parachute Drag Coefficients (Effective) and Velocities
It is not possible to do perfect analysis of the Parachute Drag coefficients because we cannot back out the drag on the mission package and booster sections. However, we can determine the effective coefficients (including the drag on these bodies).
Drogue
We trimmed the data so that it didn't include opening shock loads or main opening. We then performed analysis at two different altitudes (~7k m, ?, and ?) in order to see the difference between different altitudes.
7k-8k meters
After parsing the data between 7000 and 8000 meters and eliminating outliers, this is a scatter plot of velocity vs. altitude. Velocity was determined using backwards differentiation on a centered-moving average of 201 data points of height and time.
A normal probability plot of the velocities shows that the distribution of mission package velocity under drogue at this altitude range was approximately gaussian (similar results were shown, but not included here, for velocity squared, which is proportional to drag):
Main
Parachute Shock Loads
Drogue
Main
The Telemetrum switches the state to "main" at 298.22 seconds. Shown by the red line in the graph below, this indicates that the Raven fired the Tender Descenders first. Also shown by this graph is that main opening appears to take approximately seconds and be an approximately constant opening force (main opening is shown approximately by the dashed vertical green lines).
This is not exactly what I would expect–I would expect that as the canopy changes shape during the filling process, the opening force changes somewhat.
As you can see here, main opening took approximately 11 seconds. We can compare this with a theoretical estimate derived from the following formula (from NASA TM X-1786):
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\frac{t_{f}}{D_{o}} = \frac{0.65\lambda_{g}}{V} |
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t_{f} = \frac{0.65\lambda_{g}}{V}D_{o} |
To determine the shock force, we need to know the upwards acceleration applied by the parachute during opening (subtracting off the effect of gravity). Then we can calculate the opening shock factor using the opening shock force formula.
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For a complete Recovery analysis, please visit the Hermes I Recovery Analysis.
Parachute Drag Coefficients
E-match voltage anomaly
Post flight data review notes abnormal voltage readings on Telemetrum apogee channel. Despite commanding an apogee event, the Telemetrum continued reading 4.2V across the channel for the remainder of flight. The e-match should register a significant increase in resistance within 10 mS of exceeding it's no-fire current of no fire current here. This suggests that the initiator misfired. A fishbone analysis was conducted to classify the nature of the issue. Evidence collection is ongoing, however it appear probable that the Telemetrum e-match is internally shorted, either autogenously or to the piston.
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