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High Altitude Brayton Cycle Generators

The Missile Defense Agency (MDA) wants to demonstrate the practicability of a lighter than air (LTA) high altitude airship ("HAA") that is capable of staying aloft for more than a year at 70,000' to 80,000' carrying a multi-mission payload of up to 12,000 lb. with a nominal power requirement of 75 kW. The MDA has launched a demonstration program to serve as a stepping-stone to an operational HAA that could deploy globally from a home base. The feasibility demonstrator is required to have an endurance of one week and be capable of reaching 70,000' with a payload of 4,000 lb. and a payload power requirement of 15 kW.

High altitude LTAs are also being considered for commercial communications to complement or supplement satellites. Both missions require unmanned, long-endurance operations well above the Troposphere to avoid large amplitude atmospheric disturbances such as jet stream winds.

To achieve long endurance, solar-powered, regenerative energy systems have to be used. Power during night hours and for unusual peak daytime events is obtained from stored energy. The best approach is deemed to use hydrogen as night-time fuel that can be replenished by electrolysis during daytime hours.

The challenge is how to generate power using ambient air at altitudes where the  density has declined from 14.7 psia at sea level, to 1.05 psia at 60,000', 0.649 at 70.000', and 0.403 at 80,000'. A system arranged to operate at 60,000' may not be able to operate in an atmosphere that is less than half as dense at 80,000'.

The solution most commonly assumed to fit these requirements best is a regenerative hydrogen system based on solar-powered electrolysis to store energy for night-use in a fuel-cell. However, this approach overlooks the weight of the amount of stored oxygen required.

DARPA is conducting a feasibility demonstration program to power and propel a low earth orbit satellite with a stored hydrogen and oxygen regenerative system employing photovoltaics in combination with an electrolyzer and fuel-cell. However, since it is an orbiting satellite the cycles in darkness are short in comparison with those of a stationary airship and the weight of stored oxygen is, therefore, not as critical.

An LTA design based on stored hydrogen and oxygen can suffer severe oxygen weight penalties. Depending on reserve power requirements deemed necessary to hold station in wind storms the stored oxygen concept can be rendered unfeasible. For example, an airship designed to carry a payload of 12,000 lb up to 80,000' with the capability of withstanding a severe wind storm would need to accommodate a weight of oxygen three times greater than the entire payload.

Much of this weight penalty can be eliminated by using outside air instead of oxygen as oxidant during wind storms. The problem with a PEM fuel cell is that to use ambient air at altitude it has to be pressurized. This creates a parasitic load which escalates sharply at high altitudes. At 80,000' the pressurization system effectively overwhelms the fuel cell.

This fact stimulated CEC to design a Brayton cycle which, it believes, saves considerable weight and bulk and most likely also offers significant net system efficiency advantages at full as well as part loads.

The generation system is based on a unique form of closed Brayton cycle consisting of a two-stage turbo compressor system with intercooler, recuperator, external combustion to heat the high pressure turbine air and also to re-heat the air into the low pressure turbine. This system offers thermal efficiencies in excess of 45% over a range of power outputs from 20% to full power. This is accomplished by controlling the air density (pressure level) in the closed loop.

The external combustion system is proprietary and includes water recovery in the event that hydrogen regeneration is required. The system design provides air for combustion, re-circulates a portion of combustion gas and provides air to pressurize the closed loop.

Since fuel cells are projected to reach comparable thermal efficiencies to those of this system, the size and weight of the sink heat exchanger would be about the same for both. Excluding the weight of the heat sink exchanger, the specific weight for this form of Brayton cycle system capable of meeting the full power requirement at 80,000' would be in the order of 3.17 lb/kW (1.44 kg/Kw). With the heat sink exchanger included, comparable figures would be 4.47 lb/kW (2.03 kg/kW). At 75 kW this translates into a system weight of around 325 lb.

The system as described utilizes high speed rotating elements of reliability proven in extensive field tests of up to 10,000 hrs without failure. The two heat rejection heat exchangers are well within the state-of-the-art of aluminum manufacture, the recuperator follows design criteria that have been proven in commercial micro turbines as does the high-speed, wild frequency alternator. The novelty of the system lies in its ceramic combustion and combustion heat transfer elements and the method employed to induce air into the combustor and provide a source of air to pressurize the closed-loop. 

System Comparison:

The following is a comparison of a fuel cell and a Brayton cycle system.

The fuel cell system consists of a hydrogen/oxygen fueled, solar regenerative arrangement as illustrated in the diagram. It  consists of surface-mounted photovoltaic cells, a multiple stack electrolyzer, a multiple stack fuel cell, oxygen, hydrogen and water storage tanks and a power conditioning system. In this instance the system is sized for sustained operation at 80,000' with a constant power demand of 140 kilowatts which includes 75 kilowatts for the payload and enough thruster power to cruise at 45 knots. This part of the operation would require an electrolysis rate of roughly 400 lb of H2 per night  and 3,200 lb of O2, which implies a corresponding need for water storage of 3,600 lb at the end of each night.

The problem is that the system has to cope with occasional storms that include winds as high as 100 knots. This introduces a peak load requirement of close to 800 kilowatts. Based on an average overnight level of 700 kilowatts, the fuel cell system has a hydrogen capacity of 2,000 lb per night and corresponding oxygen consumption of 16,000 lb. At this level of energy, the complete system with solar cells included would weigh as much as 100,00 lb. Keep in mind that 13.18 cubic feet of displaced air is required to lift one pound of weight at sea level. At 80,000' that figure jumps to 480 cubic feet per pound of extra weight. Hence, to lift 100,000 pounds of system weight would require 48 million cubic feet of additional airship volume!

The solution to this problem must include reducing the stored oxygen weight which can be done by using atmospheric oxygen. The other key element in system weight reduction is to regenerate only enough hydrogen meet all but the power required to counter the most severe winds and to meet the peak storm conditions with the addition of stored compressed hydrogen.

This approach is illustrated in the adjacent system diagram.

To meet these conditions, this system could be designed with a regenerative hydrogen capacity of 660 lb per night. This cuts the size, weight and power demand of the electrolyzer about in half. The weight penalty for this system is the 1,300 lb of reserve hydrogen required to counter the worst parts of two  wind events. Including the containment weight of the hydrogen, the penalty amounts to close to 13,000 lb.

The complete systems weight for this approach is estimated to be around 50,000 lb, which at 80,000' altitude would reduce the extra airship volume from 48 to 26 million cubic feet .

High Altitude (80,000') Airship Application System Weight Comparison

 

Brayton Cycle

Fuel Cell

  Item Weight Item Weight
Electrolyzer Capacity - lb/Hr 110.2   230.4  
Electrolyzer Weight - lb/lbH2/hr** 150.0   150.0  
Electrolyzer Weight - lb   16,528.4   34,565.2
O2 Generated - lb     16,631.3  
O2 Containment Weight - lb     18,397.4  
Total O2-related Weight - lb       35,028.7
H2 consumed - lb 2,015.6   2,078.9  
H2 containment weight - lb 17,837.2   18,397.4  
Total H2-related weight - lb   19,852.8   20,476.4
H2O used/average daily weight - lb 5,950.2 2,975.1 18,710.2  
H2O containment weight - lb   734.8 4,677.5 4,677.5
Fuel Cell Weight - lb/kW     4.8  
Fuel Cell Weight - lb       3,773.3
Brayton Cycle Weight - lb/kW 3.8      
Brayton Cycle Weight - lb   2,947.9    
PV installed Weight - lb   1,482.3   1,482.3
Installation & Controls - lb   8,609.6   19,704.2
Total System Weight - lb   53,139.9   119,707.6
Volume Impact-million cu ft   25.6   57.6

** The specific weight of electrolyzers is still a long way from getting down as low as 150 lb/lb of hydrogen/hr.

The same rationale when applied to very high altitude airplanes produces similar results. Instead of airship volume, the battle becomes wingspan and since an airplane has greater forward velocity there is a beneficial level of dynamic pressure to make things a bit easier. Basically, the approach described for the airship helps to solve the power problem for any high altitude platform with long endurance requirements.