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©M. S. Ramaiah University of Applied Sciences 1 lty of Engineering & Technology Session Speaker M. Sivapragasam Session 08 Aircraft Manoeuvrability

ACD505 Session 08

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230510254Thrust is the force which moves any aircraft through the air. Propulsion system is the machine that produces thrust to push the aircraft forward through air. Different propulsion systems develop thrust in different ways, but all thrust is generated through some application of Newton's third law of motion. A gas (working fluid) is accelerated by the engine, and the reaction to this acceleration produces the thrust force. Further, the type of power plant to be used in the aircraft depends on four important factors, namely: the aircraft mission, over all weight, flying range and endurance and altitude of flight. This assignment work was partitioned into three different parts (A, B and C respectively). In Part-A, a debate was made on the viability of implementation of twin engine propulsion system for long range civil aircrafts. Logical arguments based on literatures collected from various internet and text book sources were made and the conclusion of the usage of twin engine propulsion system for long range civil aircrafts was drawn. In Part-B, for the given mission of the aircraft, suitable power plant was chosen (Turbo fan engine) and corresponding cycle analysis calculations was done. The calculations were repeated for a range of flying altitudes and performance plots drawn were critically examined. Also, for the given Turbo prop engine data, cycle analysis calculations were done. The calculations were repeated for a set of Mach numbers and performance plots drawn were critically examined. The different engine installation techniques for a turboprop engine was also discussed. In Part-C, flow over an axial gas turbine cascade was analysed in Ansys-FLUENT software package. The blade geometry was created in Ansys-BladeGen and then imported to CATIA to create the flow domain. Meshing of the geometry was done in Fluent-ICEMCFD. The total momentum thrust and propulsion efficiency for the selected turbofan engine for the extreme altitudes of 4km & 18km was estimated as 73541N & 9375N and 47% & 40% respectively. The percentage of cold thrust generated at 4km & 18km was 60% & 45% respectively. Both momentum thrust and propulsion efficiency of the engine was observed to decrease with increase in altitude. The propeller thrust and power for the given turboprop engine for flight Mach corresponding to 0.1 & 0.8 was estimated to be 191669N & 25546N and 6074467W & 6477144W respectively. With increasing Mach number of flight, propeller thrust and power was observed to decrease and increase respectively. For the flow analysis over the axial turbine cascade, maximum static pressure value occurs for +150 (2.67*105 Pa) and minimum for 00 (2.5*105 Pa) flow incidence angles respectively. The maximum Mach number value occurs for +150 (1.89) and minimum for -150 (1.57) flow incidence angles respectively. Further the pressure loss was observed to be minimum for -150 (0.1118) flow incidence angle and maximum for +150 (0.2538) flow incidence angle.

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Session Speaker M. SivapragasamSession 08Aircraft ManoeuvrabilityM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologySession ObjectivesAt the end of this session, student will be able to: Define manoeuvrability of an aircraftExplain the handling characteristics of an aircraftEstimate control surface effectivenessEstimate hinge momentsEstimate stick forcesDescribe control reversal

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvrabilityManoeuvre is an airplane executing aerobatics in a the sky Or multiple airplanes engaged in aerial combat Generally Manoeuvres are difficult to quantify, especially in an analytical framework.Basically, most manoeuvres are comparatively mundane and simply involve changing from one trimmed flight condition to another.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvrabilityWhen a pilot wishes to manoeuvre away from the current flight condition he applies control inputsThis upsets the equilibrium trim state by producing forces and moments to manoeuvre the aeroplane toward the desired flight condition.The temporary out of trim forces and moments cause the aeroplane to accelerate in a sense determined by the combined action of the control inputs.Manoeuvring flight is also referred to as accelerated flight Airframe during such flight is subjected to temporary, or transient, loads M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvrabilityThe main aerodynamic force producing device in an aeroplane is the wing,Wing lift acts normal to the direction of flight in the plane of symmetry. Normal manoeuvring involves rotating the airframe in roll, pitch and yaw to point the lift vector in the desired direction Simultaneous adjustment of both angle of attack and speed enables the lift force to generate the acceleration to manoeuvre.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvre ExampleDuring turning flight the aeroplane is rolled to the desired bank angle Horizontal component of lift causes the aeroplane to turn in the desired direction. Simultaneous increase in pitch is required to generate more lift such that the vertical component is sufficient to balance the weight of the aeroplane.to maintain level flight in the turn.

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvre ExampleWhen the pilot pulls back stick the aeroplane pitches up to generate an increased lift force this results in out-of-trim normal acceleration the pilot senses the change in acceleration.The pilot senses what appears to be an increase in the weight through increase g and is said to be pulling g.If the increased acceleration is in the direction of existing acceleration , then it is called +gIf it is against then it is called -gPilots can withstand larger +g ( 6-8) than -g (2-3)M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvre stabilityStandard definition of stability implies that when aircraft is disturbed from Trim it should recover Trim conditionHowever, during manoeuvre pilot deliberately causes it to go out of trim.Accelerations are continually varying in all directions, the analysis becomes very involvedHence analytical formulations have been developed where the acceleration is constant.Manoeuvres which can be flown at constant normal acceleration are the inside or outside loop and the steady banked turn.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvre stabilityFor the purpose of analysis the loop is simplified to a pull-up,This is just a small segment of the circular flight path.Since the steady acceleration is constrained to the plane of symmetry the problem simplifies to the analysis of longitudinal manoeuvre stabilityThe motion is steady, hence the analysis is a simple extension of that applied to longitudinal static stabilityM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyHandling Analysis leads to the concept of the longitudinal manoeuvre margin,the stability margin in manoeuvring flight,And control parameters like stick movement per g and stick force per g.Manoeuvrability of an airframe is a critical factor in its overall flying and handling qualities. Large manoeuvre stability means that large control displacements and forcesLow value could lead to the pilot overstressing the airframeM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyPhases of Flight

Radial Force = m* v 2 / r ; accn = v2 / r = n*g

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologySteady Pull-up Manoeuvre An aeroplane flying in level flight at speed V0 is subject to a small elevator input which causes it to pull up with steady pitch rate q. (see figure below)

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologySteady Pull-upIn order to sustain flight in the vertical circle it is necessary that the lift L balances not only the weight mg but the centrifugal force alsoLift is greater than the weight and L = nmg, where n is the normal load factor.This load factor quantifies the total lift necessary to maintain the manoeuvre and in steady level flight n=1.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologySteady Pull-upThe centrifugal force balance is therefore given by L mg = mV0qIncremental normal load factor is : n = (n 1) = V0q / gAircraft is pitching up steadily the tail plane experiences an increase in incidence T due to the pitch manoeuvre (see figure)For perturbations and eliminating q we get

n*m*g m*g = m *V0* q m*g(n-1) = m* V0* qM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyEffect on Tail plane

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyManoeuvrabilityIn steady level flight velocity V 0 is to usual variables C L w lift coefficient etc

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyPitching moment equation

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & Technology

Pitching moment equation M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & Technology

Pitching moment equation M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & Technology

Pitching moment equation M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStick Fixed Manoeuvre point

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStick Fixed Manoeuvre Stability

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyCoupled Effects

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyDutch RollSome of our Gliders show this !!

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStability Derivatives

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyControl Surface Deflections

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyControl Surface Effectiveness : Flap Example

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyHinge Moments

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyEstimation of Stick Forces

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStick Fixed and Stick Free

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyFixed and Free Margin

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStick Force

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyControl Issues : Aileron Reversal

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyControl Types

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyTypes of Control Systems

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyDeviations from our assumptionsAssumed linear aerodynamicsLift coefficient CL depends on linearlyNot valid for higher AOAIgnored compressibility effectsNowhere dependence on Mach number includedFor M> 0.7 has to be consideredAssumed aircraft as a rigid bodyNo deformation of aircraft components under all load conditionsM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyHigh speed effectsLift curve slope a varies drastically near M=1Aerodynamics centre a.c shifts backwardsCm0 becomes more +ve while for zero lift increases

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyAero-elastic effectsEffect of aero elasticity is to reduce lift curve slope, proportional to dynamics pressureCombined M and aero elastic effects are shown above

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyFly-By-Wire BasisIf the computer has final authority on the commands sent to the control system. The pilots inputs should be limited by the computer (hard limits or protections) to prevent exceeding the physical design limits of the aircraft (e.g., angle of attack, g loads, etc.) to protect the integrity and dynamics of the aircraft.If the pilot has final authority of the commands sent to the control system.The computer should monitor the pilots inputs for limits (soft limits) and warn when they exceed the physical design limits of the aircraftBut carry out the commands even if that would endanger the aircraft integrity or flight.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyStability and Controllability

M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyHandling QualitiesControls must feel right to pilotControl parameters (gains, damping, etc.) are unique to each aircraft and thus must be tuned typically through wind tunnel and flight testsM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyHigh AOA ProblemsModern combat aircraft fly at very high AOA and these are associated with some issues which need to be addressed.Wing Rock Roll and Yaw DivergenceM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyWing RockWing rock phenomenon is manifested by a limit cycle oscillation predominantly in roll about the body axis.This self-induced rolling oscillation is highly annoying to the pilot and poses serious limitation to the combat effectiveness.The maneuvering envelope of an aircraft exhibiting this behavior is also seriously restricted maximum angle of attack (AOA) is often limited by the onset of wing rock before the occurrence of stall.In addition, the wing rock can be a safety problem during landing. M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyWing RockThe final state is generally stable and characterized by both large roll attitudes and coupling with directional modes.Handling qualities are obviously compromised and the maneuvering capabilities degrade in terms of the maximum achievable angle of attack.Moreover the presence of wing rock in the approach or landing phase can have very serious consequences on the operational safety of the aircraft.This phenomenon, arising from a nonlinear aerodynamic mechanism.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyWing RockHas been documented in flight at a high angle of attack.On configurations with slender forebodies and highly swept wing plan forms combined with leading edge extensionsHigh speed civil transport and combat aircraft can fly under conditions where this self-induced oscillatory rolling motion is observed.The aerodynamic regime on these configurations is dominated by vortical flows. During wing rock oscillations, the normal position in the cross-flow plane of vortex cores is affected by hysteresis.M. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologyRoll and Yaw DeparturesThe roll reversal phenomenon is one in which the aircraft rolls in the opposite direction to aileron input.The roll due to adverse yaw overpowers the proverse roll due to ailerons. The directional instability/directional departure may cause the aircraft to depart from controlled flight and enter into a spin. Whether the aircraft can develop a steady spin depends on the balance between the inertial and aerodynamic momentsM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & TechnologySummaryIn this session following topics were discussed:Manoeuvrability of an aircraftHandling characteristics of an aircraftEstimation of control surface effectivenessEstimation of hinge momentsEstimation of stick forcesControl reversalM. S. Ramaiah University of Applied Sciences#Faculty of Engineering & Technology