indra poster 2.7

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Ionization Nexus for Discharge Research in the Atmosphere J. Collins 3 , V. Fernandez-Kim 4 , S. Harb 3 , B. Stutzman 3 , A. Linson 1 , J. Ozenua 2 , J. Villien 4 LaACES Project 1 Department of Civil Engineering at Louisiana State University, Baton Rouge, LA 2 Department of Petroleum Engineering at Louisiana State University, Baton Rouge, LA 3 Department of Electrical and Computer Engineering at Louisiana State University, Baton Rouge, LA 4 Department of Mechanical Engineering at Louisiana State University, Baton Rouge, LA Abstract Acknowledgements Results Conclusions The goal of the Ionization Nexus for Discharge Research in the Atmosphere (I.N.D.R.A.) experiment was to measure the breakdown voltage of the atmosphere in an effort to validate Paschen’s Curve. Paschen’s Curve is a relationship between the breakdown voltage as a function of air pressure and the distance of the electrodes. Theoretically, a decrease in pressure should correspond to a decrease in breakdown voltage. I.N.D.R.A.’s goal was accomplished by using a spark generation system to create and detect a voltage breakdown across high voltage electrodes exposed to the atmospheric conditions to an altitude of 100,000 feet. It was possible to determine the breakdown voltage of the atmosphere using INDRA’s spark gap system. The payload was successfully launched on May 20, 2014 from NASA’s Columbia Scientific Balloon Facility in Palestine, Texas. The decreasing pressure did show a correlation with increasing breakdown voltage on both the ascent and decent. This correlation was within 66% confidence, which was a mission goal. However, due to an unexpected dip in breakdown voltage, this experiment should be repeated to confirm results. Further work is also warranted to study the relationship between atmospheric humidity and temperature on breakdown voltage. Payload Design Arc Detection Board Analysis October 4, 2014 Supported by the Louisiana Space Consortium. Special thanks to the LaACES Staff: T. G. Guzik, D. Granger, M. Stewart, B. Ellison, C. Fava, J.P. Wefel, D. Browne, and the staff of the NASA Columbia Scientific Ballooning Facility Software System Flowchart 0.001 0.01 0.1 1000 1500 2000 2500 3000 3500 Paschen's Curve (Ascent) Pressure*Distance (bar*cm) Breakdown Voltage (V)

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Page 1: Indra Poster 2.7

Ionization Nexus for Discharge Research in the AtmosphereJ. Collins 3, V. Fernandez-Kim4, S. Harb 3, B. Stutzman 3, A. Linson 1, J. Ozenua 2, J. Villien4

LaACES Project

1 Department of Civil Engineering at Louisiana State University, Baton Rouge, LA 2 Department of Petroleum Engineering at Louisiana State University, Baton Rouge, LA 3 Department of Electrical and Computer Engineering at Louisiana State University, Baton Rouge, LA 4Department of Mechanical Engineering at Louisiana State University, Baton Rouge, LA

Abstract

Acknowledgements

Results

Conclusions

The goal of the Ionization Nexus for Discharge Research in the Atmosphere (I.N.D.R.A.) experiment was to measure the breakdown voltage of the atmosphere in an effort to validate Paschen’s Curve. Paschen’s Curve is a relationship between the breakdown voltage as a function of air pressure and the distance of the electrodes. Theoretically, a decrease in pressure should correspond to a decrease in breakdown voltage. I.N.D.R.A.’s goal was accomplished by using a spark generation system to create and detect a voltage breakdown across high voltage electrodes exposed to the atmospheric conditions to an altitude of 100,000 feet.

It was possible to determine the breakdown voltage of the atmosphere using INDRA’s spark gap system. The payload was successfully launched on May 20, 2014 from NASA’s Columbia Scientific Balloon Facility in Palestine, Texas. The decreasing pressure did show a correlation with increasing breakdown voltage on both the ascent and decent. This correlation was within 66% confidence, which was a mission goal. However, due to an unexpected dip in breakdown voltage, this experiment should be repeated to confirm results. Further work is also warranted to study the relationship between atmospheric humidity and temperature on breakdown voltage.

Payload Design

Arc Detection Board

Analysis

October 4, 2014

Supported by the Louisiana Space Consortium. Special thanks to the LaACES Staff: T. G. Guzik, D. Granger, M. Stewart, B. Ellison, C. Fava, J.P. Wefel, D. Browne, and the staff of the NASA Columbia Scientific Ballooning Facility

Software System Flowchart

0.001 0.01 0.11000

1500

2000

2500

3000

3500Paschen's Curve (Ascent)

Pressure*Distance (bar*cm)

Bre

akdo

wn

Vol

tage

(V)

0.001 0.01 0.11000

1500

2000

2500

3000

3500

4000

4500Paschen's Curve (Descent)

Pressure*Distance (bar*cm)

Bre

akdo

wn

Vol

tage

(V)

1 10100

1000

Pressure ∙ Distance (bar∙cm)

Vol

tage

(V)

Potential Expected Data Voltage vs Pressure Distance

0 20000 40000 60000 80000 100000 1200001500

2000

2500

3000

3500

4000

4500 Breakdown Voltage vs Altitude (Ascent)

Altitude (ft)

Bre

akdo

wn

Vol

tage

(v)

30000 35000 40000 45000 50000 55000 60000 65000 70000 75000 800001500

2000

2500

3000

3500

4000

4500Breakdown Voltage vs Altitude (Descent)

Altitude (ft)

Bre

akdo

wn

Vol

tage

(v)

Prior to flight, the INDRA team created a table of expected results, mapped across the range of expected pressures for flight. The recorded flight data matched the general trend of our expected data: a decrease in pressure yielded a decrease in breakdown voltage. However, INDRA observed one notable exception to this trend, visible on the Ascent breakdown voltage curve. Although the exact cause for the dip is unknown, possible causes include condensation on the electrodes, dislodged foam, or signal interference from the arc discharges. The decent records match more closely with expected values.

Start: Initialize datavariables

ADC ReadRoutine

AtmosphericPressure

Check

Set DAC to 0.

HVDC RampRoutine

EEPROMWrite routine

EEPROMMemoryCheck

Payload Containment Unit Design

Principle of OperationThe payload is controlled in real-time using a BASIC Stamp processor. A high voltage is applied across a pair of high voltage electrodes (the ‘spark gap’). The voltage is raised in 15V increments until the voltage exceeded the breakdown voltage of the atmosphere, which forms an arc between the electrodes. The payload then detects the arc and records the breakdown voltage into an onboard memory chip. The payload is constructed using lightweight foam and wood.

Spark Generation System