High Altitude Operations with Piston Engines Power Plant Design Optimization Part I: Introduction
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VOL. 11, NO. 5, MARCH 2016 ISSN 1819-6608 ARPN Journal of Engineering and Applied Sciences ©2006-2016 Asian Research Publishing Network (ARPN). All rights reserved. www.arpnjournals.com HIGH ALTITUDE OPERATIONS WITH PISTON ENGINES POWER PLANT DESIGN OPTIMIZATION PART I: INTRODUCTION Luca Piancastelli, Leonardo Frizziero, Simone Pica and Giampiero Donnici Department of Industrial Engineering, Alma Mater Studiorum University of Bologna, Viale Risorgimento, Bologna, Italy E-Mail: [email protected] ABSTRACT Diesel and spark-ignition piston engines are an ideal choice for long endurance, high altitude operations (10, 000m/33, 000ft) and extremely high altitude operations (20,000m-65,000ft). These systems are more complex than traditional applications that are normally limited to 5, 000-7, 000m (16, 000-23, 000ft). In fact, the air propulsion system (propeller or fan), the air intake, the fuel system, the turbo charging, the exhaust and the cooling system take part to the design optimization process. An integrated design is strictly necessary. Since prop-fan is currently under development, the design should start from the choice between propeller and fan. This choice will influence optimum cruise speed, critical altitude and aircraft design as a whole. The air induction system is extremely important to improve efficiency, endurance and critical altitude. At low altitude, a filtered induction system is used for takeoff. At high altitudes, the intake air is taken from high-pressure areas into an alternate, extremely optimized, path. This induction system recovers as much pressure as possible, air kinetic energy at cruise speed. In propeller systems, the intake is usually positioned in the lower part of the aircraft. On fan systems, a little amount of “high pressure” air is taken from the high-pressure area of the fan. The exhaust system is also critical with the choice between pressure recovery and thrust. Exhaust-pressure-recovery reduces backpressure and temperature at exhaust. However, the improvement in critical altitude is marginal. In more common, thrust driven exhaust systems, the exhaust energy is converted into speed and thrust. At the relatively high speed of high altitude cruise, also the cooling system adds a small amount of thrust through the Meredith’s effect. The piston engine power plant design is then extremely critical. Many different components should find the correct position for maximum performance. The power-plants of WWII water-cooled fighters and bombers are good examples, even if their design cruise altitude is below 10, 000m (33, 000ft). Modern turbofan and turbojet air intakes are also of help. However, the requirements of low weight, high reliability and long endurance HALE (High Altitude Long Endurance) UAVs (Unmanned Aerial Vehicle) requires further work on this specific subject. Keywords: optimization, HALE, UAV, thruster, cooling, meredith effect. INTRODUCTION fuel consumption and provide range. Mach 0.9 represents Propulsion system is a most difficult technical the approximate upper speed limit for a subsonic fan challenge in unmanned aircraft designed to fly propelled aircraft, while Mach 0.4 represents the subsonically >20, 000m (60, 000ft) for >4 hrs. In this theoretical best efficiency aircraft speed. Subsonic slow flight regime, however, air breathing propulsion is difficult flight at altitudes >20, 000m favour thrusters with to achieve due to the small air density and pressure with relatively large actuator areas (i.e. a propeller driven altitude. Turbochargers (TC) are needed to supply most of aircraft), and the actuator size (i.e. propeller diameter) will the intake pressurization required to compress ambient air approximately 3 times larger than medium altitude into the intake. Volume flow requirements increase with conventional aircraft (5, 000m). altitude, which translates to larger TC size. Pressure ratio Beyond certain power levels (≈200kW), the fan requirements also increase with altitude, which translates replaces the propeller. Because of the increased size and to more TC stages. Since power is proportional to airflow weight of the air handling system and thrust delivery for any air breathing engine, the powerplant size required components, a propulsion system optimized for high to process airflow for a rated power will grow. Interstage altitudes is significantly larger and heavier than its low and afterstage cooling is required for efficiency and power altitude counterpart. Moreover, the HALE (High Altitude output. Weight is proportional to the cube of linear Long Endurance) vehicle needs more power to stay aloft. dimensions. Theoretically, heat exchanger sizing is driven In fact, faster flight speeds are necessary to maintain upwards by the reduced convective heat transfer available, dynamic pressure and support its weight in low density air. and the lower density ambient air. Practically, Meredith Therefore, the propulsion system claims greater fractions cooling duct will partially recover pressure and will output of the airplane's gross weight. This runs counter to the additional thrust. The very low OAT (Outside Air airplane's ability to carry the necessary fuel weight and Temperature) of -56.5 DEC C also helps the cooling payload. In this first part of the paper the choice between system. However, flying subsonically in low density air propeller and fan, the air induction, the exhaust and the requires larger thruster "capture/actuator-disk" areas to cooling systems are discussed, since they are most critical achieve the propulsive efficiency that is needed to reduce for HALE UAVs optimization. 3525 VOL. 11, NO. 5, MARCH 2016 ISSN 1819-6608 ARPN Journal of Engineering and Applied Sciences ©2006-2016 Asian Research Publishing Network (ARPN). All rights reserved. www.arpnjournals.com Propulsion system: propeller or fan As part of the ERAST (Environmental Research Aircraft and Sensor Technology) 1987-2003 programs, NASA started developing an UAV (Unmanned Aerial Vehicle) for chemical analysis in the stratosphere. The requirements for the propulsion system, consisted in an altitude of 25.9 km, and an absorbed propeller power of 63.4 kW (85 hp), at a cruise velocity of Mach 0.4. A propeller was then designed with Glauert’s momentum- blade element theory and with the ADPAC (Advanced Ducted Propfan Analysis Code) program, a CFD code. Figure-1. Propeller for 190kW/1250rpm/20km/0.4 M/ The final design was a 4.6 meters diameter three- 2.5m diameter. bladed propeller. The airfoil used for the sections was the Eppler 387, which is optimum for low Reynolds numbers, although it is slightly thicker than the modern transonic In order to simplify the construction the power airfoils, with could create problems due to compressibility was split into two propulsion units as shown in Figure-2. effects near the tip and to moisture/ice in air. The Eppler The quite large blended fuselage was due to the circular 387 was previously tested. The tests at the NASA Langley satellite communication antenna. Low Turbulence Pressure Tunnel provided very high quality data in the range of 0.015–0.2 Mach. The 85.1% propeller efficiency of Glauert’s theory was similar to the one obtained from CFD simulation (86.2%). However, a propeller of this size, although it presents a good efficiency, causes serious problems of installation. In 2006, a contra-rotating propeller was designed for a vehicle capable of flying at an altitude of 25 km. The absorbed power can range from 110 kW to 220.5 kW at 0.4-0.7 M. Table-1. Contra-rotating propeller data. D (m) N (rpm) P (kW) ηi Figure-2. High altitude (20, 000m) UAV preliminary 2.5 1,250 190 86% design with two contra-rotating propulsion units. The application of Theodorsen’s theory for Theoretically, it is possible to design high-speed contra-rotating propellers led to the choice of a 2.5 m six propellers, called propfans that NASA developed until bladed propeller, which can be observed in Figure-1. The 1990. This program saw recently new interest due to high propellers rotate at 1250 rpm and absorb a power of fuel price. However, the propfan has encountered several 183.75 kW, with an induced efficiency of 87.6%. This problems of noise and turbulence that have not been larger value of the induced efficiency is due to the higher solved. For practical reasons a (shrouded) fan is the best value of the power and rotational speed, which could not choice for power levels higher than [email protected]/25km. be adopted with a single-rotating propeller, because of the Figure 3 shows a fan designed for a 200kW-20, 000m- excessive value of induced speed and the consequent 0.4M-UAV. The diameter of the fan is 0.29m (11-in.). decrease of efficiency. The other characteristics of the This fan is based on NASA CR2003-212369 design. dual-rotating propeller are shown in Table-1. These Propulsion efficiency is defined by equation (1) evaluations were substantially confirmed by Solid Work CFD simulation, although the efficiency proved to be 2 (1) slightly lower (86%). p c 1 v While thrust T is given by equation (2). D2 T vc v (2) 4 3526 VOL. 11, NO. 5, MARCH 2016 ISSN 1819-6608 ARPN Journal of Engineering and Applied Sciences ©2006-2016 Asian Research Publishing Network (ARPN). All rights reserved. www.arpnjournals.com For the same thrust T, ve is larger for the fan than possible to reach higher density altitude where engine for the propeller, since the diameter D of the fan is smaller power output is reduced. An advantage of diesel over than the diameter of the propeller for the same absorbed spark ignition engines that the efficiency is kept almost power (2). For this reason, in order to have the same equal even at extremely reduced power output. In the case propeller efficiency (1), the fan-propelled aircraft should of spark-ignition engines efficiency is slightly reduced be faster than the propeller-propelled aircraft.