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Development of High Altitude Sprite Imagery Capability - Bruski

Development of High Altitude Sprite Imagery Capability - Bruski

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United States Air Force Academy’s Meteorology Department. The flight reached a maximum altitude <strong>of</strong> 31 km and<br />

landed approximately 88 km north and east <strong>of</strong> the launch location. The unit was recovered successfully with the help<br />

<strong>of</strong> a last second SPOT® tracker unit from a local high school.<br />

B. Flight Two<br />

Flight two was a test <strong>of</strong> the SPOT® tracker at high altitudes, a new payload box, and a new parachute. The<br />

balloon flight was a launch and forgets mission since no live data was being sent down to the ground. The flight<br />

landed approximately 125 miles north and east <strong>of</strong> its launch location. The balloon was recovered at 11 pm in zero<br />

light conditions.<br />

C. Flight Three<br />

Flight three served as a test <strong>of</strong> the HD GoPro Hero Naked® video camera. The camera was pointed straight<br />

down to demonstrate that position for future flights. The flight also demonstrated the necessity <strong>of</strong> having a<br />

redundant tracking system as the APRS feed was lost when the balloon was approximately 762 meters in altitude.<br />

The SPOT® tracker successfully sent its position to the tracking website 170 miles from the launch site. The balloon<br />

was in the air for over four hours which contributed to the extreme distance the balloon landed from the launch site.<br />

A unusual wind pattern at 30 km was identified. Winds usually are calm at 30 km however, on this occasion the<br />

balloon picked up speed reaching a maximum velocity <strong>of</strong> 104.60 km per hour at 31 km in altitude.<br />

D. Flight Four<br />

Flight four served as a test for a new GPS receiver unit and to demonstrate a new flight pr<strong>of</strong>ile used to track<br />

balloons near thunderstorms. This flight was unique in that it used almost exactly the same materials as the last<br />

flight to demonstrate rapid reuse and low turnaround time. A more accurate method <strong>of</strong> measuring lift was developed<br />

to guarantee a short flight. 4.54 kg <strong>of</strong> weights were tied to the bottom <strong>of</strong> the balloon which was then filled until they<br />

could be lifted <strong>of</strong>f the ground. Approximate lift was 11 pounds at launch. At about 35 minutes into the flight and at<br />

an altitude <strong>of</strong> 17 km extreme turbulence was encountered. This combined with a small amount <strong>of</strong> ice buildup on the<br />

cord connecting the parachute to the payload box led to the payload box separating from the balloon and parachute.<br />

The payload box survived a free fall from 17 km to impact at almost 112.63 km per hour with little to no damage.<br />

Again, this flight demonstrated a need for a redundant tracking system as the violent force <strong>of</strong> the impact caused the<br />

SPOT tracker to turn <strong>of</strong>f. The box was located using previous data points to calculate descent rate and then<br />

combined with the winds that day to draw a probability circle to where it landed. The system was still transmitting<br />

its position 24 hours later which was picked up by HAM radio and when entered into a handheld GPS led straight to<br />

its recovery site.<br />

VI. Future Test Flights<br />

Two final test flights remain before the system is considered operational. The first test will demonstrate the<br />

ability <strong>of</strong> the system to successfully cut the balloon away from the parachute using a HAM radio to send a signal to<br />

a receiver onboard the balloon. This signal will be in the form <strong>of</strong> a coded sequence <strong>of</strong> numbers that will be read by a<br />

DTMF (dual tone multi-frequency) board and will activate a relay switch. This switch will allow current to flow<br />

through a nichrome wire wrapped around the nylon cord connecting the balloon to the parachute. With the current<br />

flow, the wire will heat up and melt through the string in a matter <strong>of</strong> seconds. In all previous flights, the balloons<br />

have failed to shred as they are designed to do at altitude. They remain mostly intact as 2-3 kg <strong>of</strong> dead weight above<br />

the parachute causing it to only partially inflate enter into a fast than expected fall. The cut down system will allow a<br />

precise maximum altitude and a more predictable landing site. Finally the second test flight that remains will serve<br />

as a test <strong>of</strong> the high altitude long duration flight at a relatively stable position. Through previous flights and the<br />

advice <strong>of</strong> the USAF Academy Meteorology Department, a region at approximately 18-21 km has been found to<br />

contain winds that are below 16.09 km per hour. This altitude is ideal for long duration flights as it is high enough to<br />

be above most <strong>of</strong> the atmospheric distortion and out <strong>of</strong> the winds. Should this region not prove to be calm, the flight<br />

will continue to rise until a calm region is found. At launch, the flight will consist <strong>of</strong> two balloons connected<br />

separately to the payload box. The large main balloon will be filled to the point where its lift exactly matches the<br />

weight <strong>of</strong> the payload and the system will be neutrally buoyant. The second smaller balloon will simply to provide<br />

the lift needed to get the system up to the desired altitude. A separate cut down device will be connected to each <strong>of</strong><br />

the balloons and at that desired altitude, the balloon providing the free lift will be cut away and the system will<br />

4<br />

American Institute <strong>of</strong> Aeronautics and Astronautics

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