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A report by A report by Darshak Bhuptani

Aerodynamics of a_rotary_wing_type_aircraft

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how helicopter flies!!

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Page 1: Aerodynamics of a_rotary_wing_type_aircraft

A report byA report byDarshak Bhuptani

Page 2: Aerodynamics of a_rotary_wing_type_aircraft

Introduction to basic aerodynamics

� Newton's Laws of Motion� Fluid flow and Airspeed measurement. (Bernoulli’s

Principle)

Page 3: Aerodynamics of a_rotary_wing_type_aircraft

Venturi Effect

Page 4: Aerodynamics of a_rotary_wing_type_aircraft

Rotary wing plan forms

Page 5: Aerodynamics of a_rotary_wing_type_aircraft

Terminology used for rotor� Chord (1)� Span (2)� Vertical Hinge Pin (3)

Horizontal Hinge Pin (4)� Horizontal Hinge Pin (4)� Trunnion (5)� Yoke (6)� Blade Grip Retainer Bearings (7)� Blade Twist

Page 6: Aerodynamics of a_rotary_wing_type_aircraft

Airfoils in general

Applications:� Sustentation (A Wing or Rotor Blade) � For Stability (As a Fin)

For Control (A Flight Surface, such as a Rudder) � For Control (A Flight Surface, such as a Rudder) � For Thrust (A Propeller or Rotor Blade)

aerodynamic forces necessary to keep any body aloft are produced when air passes about the rotor blades and this is known as “Lift”

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Airfoil Terminology

Page 8: Aerodynamics of a_rotary_wing_type_aircraft

Pressure patterns on the airfoil

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Lift for a symmetrical airfoil

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Relative wind

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How still air is changed to a column of descending air by rotor blade actiona three-bladed system rotating at 320 revolutions per minute passes a given point in the tip-path plane 16 times per second

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Airflow from rotation, modified by induced flow, produces the Resultant Relative Wind.

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Centrifugal force & Centripetal Force� Because of its rotation and weight, the rotor system is

subject to forces and moments peculiar to all rotating masses. One of the forces produced is Centrifugal Force.Force.

� It is defined as the force that tends to make rotating bodies move away from the centre of rotation.

� Centripetal Force. It is the force that counteracts centrifugal force by keeping an object a certain radius from the axis of rotation.

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The effective diameter of the rotor disk with increased coning is less than the diameter of the other disk with less coning. A smaller disk diameter has less disk diameter has less potential to produce lift

Page 15: Aerodynamics of a_rotary_wing_type_aircraft

Gyroscopic Precession

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Drag forcesTotal Drag produced by an aircraft is the sum of the Profile drag, Induceddrag, and Parasite drag

Curve "A" shows that parasite drag is very low at slow airspeeds and increases with higher airspeeds.

Curve "B" shows how induced drag decreases as aircraft airspeed increases

Curve "C" shows the profile drag curve. Profile drag remains relatively constant throughout the speed range with some increase at the higher airspeeds.

Curve "D" shows total drag and represents the sum of the other three curves. It identifies the airspeed range, line "E", at which total drag is lowest. That airspeed is the best airspeed for maximum endurance, best rate of climb, and minimum rate of descent in autorotation.

Page 17: Aerodynamics of a_rotary_wing_type_aircraft

Torque� The helicopter fuselage tends to rotate in the direction

opposite to the rotor blades. This effect is called torque.� The torque effect on the fuselage is a direct result of the

work/resistance of the main rotor� Compensation for torque in the single main rotor

helicopter is accomplished by means of a variable pitch anti-torque rotor (tail rotor)

� the tail rotor produces thrust in a horizontal plane opposite to torque reaction developed by the main rotor.

Page 18: Aerodynamics of a_rotary_wing_type_aircraft

� From 5 to 30 percent of the available engine power may be needed to drive the tail rotor depending on helicopter size and design.

� A helicopter with 9,500 horsepower might require 1,200 horsepower to drive the tail rotor1,200 horsepower to drive the tail rotor

� a 200 horsepower aircraft might require only 10 horsepower for torque correction.

Page 19: Aerodynamics of a_rotary_wing_type_aircraft

Translating Tendency

� During hovering flight, the single rotor helicopter has a tendency to drift laterally to the right due to the lateral thrust being supplied by the tail rotor.

� The pilot may prevent right lateral drift of the � The pilot may prevent right lateral drift of the helicopter by tilting the main rotor disk to the left

� This lateral tilt results in a main rotor force to the left that compensates for the tail rotor thrust to the right.

Page 20: Aerodynamics of a_rotary_wing_type_aircraft

Angle of attack� The angle between the airfoil chord line and its direction

of motion relative to the air (the resulting Relative Wind)

Page 21: Aerodynamics of a_rotary_wing_type_aircraft

Angle of Incidence (or AOI)� Angle of Incidence (or AOI) is the angle between the

blade chord line and the plane of rotation of the rotor system.

� It is a mechanical angle rather than an aerodynamic angle: angle:

Page 22: Aerodynamics of a_rotary_wing_type_aircraft

Rotational velocities in the rotor system

when speed is doubled, lift is increased four times.

T

Page 23: Aerodynamics of a_rotary_wing_type_aircraft

Lift variation along the span� The lift at point "A" would be only one-fourth as much

as lift at the blade tip� Because of the potential lift differential along the

blade resulting primarily from speed variation, blades are designed with a twist.are designed with a twist.

� This graphic compares a twisted versus an untwisted blades lift:

Page 24: Aerodynamics of a_rotary_wing_type_aircraft

Dissymmetry of lift� Dissymmetry of lift is the difference in lift that exists

between the advancing half of the rotor disk and the retreating half.

� The blade passing the tail and advancing around the right side of the helicopter has an increasing airspeed right side of the helicopter has an increasing airspeed which reaches maximum at the 3 o'clock position.

� the airspeed reduces to essentially rotational airspeed over the nose of the helicopter. Leaving the nose, the blade airspeed progressively decreases and reaches minimum airspeed at the 9 o'clock position.

Page 25: Aerodynamics of a_rotary_wing_type_aircraft

Diagrammatic representation

Page 26: Aerodynamics of a_rotary_wing_type_aircraft

Factors which can be used to overcome the dissymmetry of liftIn the lift equation,� density ratio and blade area are the same for both the

advancing and retreating blades� The airfoil shape is fixed for a given blade. � The airfoil shape is fixed for a given blade. � The only remaining variables are changes in blade

angle of attack and blade airspeed.� These two variables must compensate for each other

during forward flight to overcome dissymmetry of lift

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Page 28: Aerodynamics of a_rotary_wing_type_aircraft

Blade flappingRight side of the helicopter Left side of the helicopter

Page 29: Aerodynamics of a_rotary_wing_type_aircraft

Flapping Velocity� Flapping Velocity, both upward and downward,

must be of such a value as to increase or decrease the angle of attack so that the lift will remain constant.

� The force-displacement phase is 90 degrees� the maximum upward and flapping velocity is

directly over the right side of the helicopter, the directly over the right side of the helicopter, the maximum displacement or actual flapping will take place over the nose of the aircraft.

� the maximum downward flapping velocity is directly over the left side of the helicopter, the maximum displacement or actual flapping will take place over the tail of the aircraft

Page 30: Aerodynamics of a_rotary_wing_type_aircraft

Ground effect� Ground Effect is a condition of improved performance

encountered when operating near (within 1/2 rotor diameter) of the ground.

� Increased blade efficiency while operating in ground effect is due to two separate and distinct phenomena. effect is due to two separate and distinct phenomena.

� The high power requirement needed to hover out of ground effect is reduced when operating in ground effect.

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Reasons for less power requirement� reduction of the velocity of the induced airflow.� The result is less induced drag and a more vertical lift

vector

Page 32: Aerodynamics of a_rotary_wing_type_aircraft

a reduction of the Rotor Tip Vortex

The airfoil operating out-of-ground-effect is less efficient because of increased induced wind velocity which reduces angle of attackangle of attack

The airfoil that is in-ground-effect is more efficient because it operates at a larger angle of attack and produces a more vertical lift vector

Page 33: Aerodynamics of a_rotary_wing_type_aircraft

The HoverHovering is the term applied when a helicopter maintains a constant position at a selected point, usually a few feet above the ground (but not always, helicopters can hover high in the air, given sufficient power.

The rotor blades move large volumes of air in a downward direction

This is the air flow around a hovering helicopter(Note: it is out of ground effect)

Page 34: Aerodynamics of a_rotary_wing_type_aircraft

Retreating blade stall

� The airspeed of the retreating blade (the blade moving away from the direction of flight) slows down as forward speed increases.

� as the airspeed of the retreating blade decreases with � as the airspeed of the retreating blade decreases with forward aircraft speed, the blade angle of attack must be increased to equalize lift throughout the rotor disk area.

� As forward airspeed increases, the "no lift" areas move left of centre, covering more of the retreating blade sectors.

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Page 36: Aerodynamics of a_rotary_wing_type_aircraft

The major warnings of approaching retreating blade stall conditions are:

� Abnormal Vibration � Nose Pitch up

When operating at high forward airspeeds:When operating at high forward airspeeds:High Blade loading (high gross weight) Low Rotor RPM High Density Altitude Turbulent Air

Page 37: Aerodynamics of a_rotary_wing_type_aircraft

Thank you� Any Question please ?