The principle of flight of ornithopters
An Ornithopter, or ornitotero like Leonardo da Vinci termed them, is an aircraft heavier than air, which flies like a bird by flapping its wings. The special feature lies in the wings that do not only generate lift but also thrust.
Ornithopters are mostly built the size of birds or flying models and then are also
flapping wing model.
The basic operating principle of a flapping wing has already been discovered (1889) by Otto Lilienthal . To help understanding an effective way of flying of big ornithopters his functional description is still trend-setting to the present day. Especially Alexander Lippisch (papers 1925 - 1939) and Erich von Holst (papers 1940 - 1943), as well as the research work of many biologists, have advanced the theory of the flapping flight further. But many details are still not understood.
Always there have been several different versions of the flapping flight theory. They all exist in parallel and their specifications are widely distributed. Calculating the balance of forces even of a straight and merely slowly flapping wing remained difficult to the present day. In general, it is only possible in a simplified way. Furthermore, the known drive mechanism and especially wing designs leave a lot to be desired.
In every respect ornithopters are still standing at the beginning of their design development. But powerful drives make very beautiful flights already possible.
Also here follows only a variant of the flapping flight theory in short version.
2. Operating principle of the flapping wing
- Diagram 1
- Optimized lift distributions for a gently inclined climb flight with limited wingspan
- Diagram 2
- Optimized lift distributions for a gently inclined climb flight with unlimited wingspan
On a stretched flapping wing lift is generated similar to an inflexible airfoil flown against from the front.
But during the wing upstroke the air flow hits the wing rather from above and in the downstroke rather from bottom. These modifications are small in the area of the wing root and gets bigger towards the wing tip.
With permanent changing twisting the flapping wing must adapt to these alternating incoming flow directions. Here, however, the lift distribution along the wing span must not be kept constant in the interest of generating thrust (please look at the diagrams).
During the wing downstroke the lift distribution is bigger altogether than when gliding and more displaced towards the wing tip. It is easy to imagine that thrust is generated along the whole wing span during stroke motion. This works similar to a propeller blade with a very large pitch - only that the propeller torque force that has to be overcome is here called lift and is also used like that.
- Vector diagram of forces and velocities
- Forces at the stork wing on upstroke
On the wing upstroke circumstances are reversed. Overall, the lift distribution is smaller and more shifted towards the wing root. With the stroke motion in the direction of the lift force the flapping wing now acts as a wind turbine blade. If the lift force is big enough it presses the wing upward even without a mechanical drive. Thereby, the wing operates with the operating drag or working drag, of a wind turbine against the flight direction (please takes a look at the vector diagram).
At the same time, the outboard wing areas are flown against rather from above. There indeed is generated negative lift but similar to a propeller also thrust (please look at the vector diagram).
Whether in the upstroke the wind turbine or the propeller function dominates depends on the wing twisting and on the shape of the lift distribution (for more details, please see following chapter).
- Comparison of aero-
The adjacent picture clarifies that the comparison does not apply in all respects to a propeller or to a wind turbine. The velocity proportions at the flapping wing are completely different. But the rotating machines are not designed for simultaneous lift generation. Furthermore, at the flapping wing the lift force at mid-span of the wing is never zero - as like at the rotating machines.
A flapping wing is an aerodynamic machine with two working cycles, the upstroke and the downstroke. In unaccelerated horizontal flight of a flying wing ornithopter the degree of efficiency of this machine is equal to zero. It only moves itself but emits no power.
But if you add a fuselage and a tail unit to the flying wing ornithopter, the flapping
wing must apply power to overcome the parasitic drag. Now the flapping wing renders
output. Now, paradoxically - with an otherwise unchanged flight attitude - the
efficiency factor becomes bigger than before (bigger than zero). For example the
efficiency factor of the flapping wing increases with the size of the tail unit
while keeping the balance of forces. So the parameter
is relatively inapplicable for evaluating flapping wings (please take a look at
the comparison of the transport performance).
The total thrust gets bigger the more the lift distributions of the up- and downstroke are different from each other - especially at the outboard wing area where the most working will be performed. If the difference equals zero operating drag and thrust have the same size and cancel out each other (please look at A. Lippisch 1938 and the vector diagram). The total thrust equals zero, then. At an existing lift difference the thrust is also increased with increasing flapping frequency and flapping amplitude.
For a steady flight, all forces - more precisely the force impulses (product from force and duration of action) - affecting the ornithopter during a complete wing beat cycle must be in balance. The propeller effect must not only balance the wind turbine effect but also all remaining drags of the wing and the aircraft. At the same time, the positive part of the lift must outbalance the negative to an extent, that it can carry the weight of the aircraft.
2.1. Rotation of the flapping wing
The course of the lift along the span is modified by the twisting of the flapping wing. But also a rotation of the wing at the wing root around its longitudinal axis changes the lift. The rotation of the wing only influences the size of its lift in the calculation model, but not its distribution along the span (see adjacent figure). The wing twisting must be adjusted accordingly. This would be different with the rotation of a rigid wing.
- Changes of lift with a rotation of the flapping wing during wing upstroke in the computer model
In the calculation model the rotation of the wing root is indicated starting from the glide position. It is only indirectly determined by the selection of the lift size. For this purpose, the circulation factor kΓ is used (the cirkulation factor k-Gamma describes the size of the lift in relation to that of the gliding flight). In the adjacent figure, the lift with rotation of the wing root during upstroke by about +6 degrees, amounts to almost 80 % of the gliding flight.
When rotating the wing, the required twisting becomes smaller, at least in wing upstroke (please see calculated examples in Flapping wings with and without wing rotation, in German, PDF 0.7 MB). However, the rotation is limited by the maximum permissible lift coefficient of the airfoil at the wing root. The rotation and thus the lift can be further increased by greater camber of the airfoil and/or wing depth in this area. Birds in particular use a very large camber of the airfoil.
In the generally used theory of the cruise flight of birds the rotation of the wing is not considered. Also with the older lift distributions shown above, the angle of incidence at the wing root is kept constant during the wing flapping motion (please see diagrams 1 and 2 above). The pictured differences of lift at the wing root results only from different induced downwind angles (please look at the diagram Downwash distributions).
To equalize the total lift, E. v. Holst (1943) suggests a rotation of the wing root, in addition to wing twisting. During upstroke the angle of attack near the wing root should be increased and reduced at downstroke. Based on present knowledge, however, turning should not be done at up- and down-stroke also like at my flapping wing models EV1 to EV5, but only during upstroke.
For birds in cruising flight the rotation is sometimes good to observe, especially near the lower final stroke position (see animations of a swan and a stork and the article Lift during wing upstroke, version 10.0, 2015 - 2018, PDF 1.0 MB). The thereby resulting large lift generates, so to speak, a large impulse of lift as reserve capacity. Then, the bird does not need to generate so much lift during the subsequent rapid upward motion of its wings. In this way, the wind turbine function and the resulting negative thrust of the upstroke become smaller. Nevertheless, the sum of the lift impulse will be large over the entire duration of the upstroke.
During the upstroke, so one have the following possibilities to increase the lift with the arm wing:
- Increase the angle of attack by rotation of the wing in the close-range of the lower final stroke position.
- Shift as much lift as possible to the span centre during the fast upstroke motion. By twisting and rotating of wing, however, this is only partly possible. The thereby reduced but still occurring negative thrust must be taken into account.
- Maintain the large angle of attack at the elbow in the upper final stroke position, until the hand wing is extended (see the motion sequence of the arm wing at the articulated flapping wing). This also works without rotation of the wing.
For a lift increase near the wing root birds can probably use still further possibilities. It is conceivable a mechanical coupling of the movements when bend the upper arm during wing upstroke. This could increase the angle of attack and/or the airfoil camber in the area of the elbow. Even just one activity of the tension muscle of the anterior pelvis (propatagium) would be suitable for this (please see 3D-form of the bird wing by K. Herzog). Especially with not so high demands on the lift changes or with long wings, thereby can be dispensed with the rotation of the wing root. Unfortunately, K. Herzog reports nothing about such functions of the biological wing.
When a seagull is flying with a strong headwind, her whole body swing up and down, something like at the gull in a gusty wind (0.5 MB). During its downward movement, in this way the inflow at the wing root is more from below. This increases the lift and creates thrust, please note thrust at the wing root. However, this was not yet investigated nearer, also not with other birds.
In small birds and ornithopters because of the high flapping frequency transient flow conditions prevail at the wing. Thereby the lift increases even without wing rotation in the lower final stroke position (please see site Handbook, chapter 4).
For further information about the
Rotation of the flapping wing see the
following chapter 4. How birds fly.
Very thorough observations of the bird flight and interesting ideas of the wing upstroke and the wing rotation also shows Brendan Body`s homepage, external link 1.
3. Flapping wing properties during flight
3.1 Gently inclined climb flight
At the wing upstroke the aerodynamic forces along the wing can be adjusted by suitable wing twisting so that the torsional moments round the wing hinge balanced themself (please look at the following diagram 3). Here, the wing area close to the fuselage acting as a wind turbine directly powers the outboard wing area acting as a propeller. This is the 1st possibility to use the wind turbine energy.
There is no energy consumption or transfer at this upstroke configuration. The wing can virtually be flapped up by the drive without effort. Propeller and wind turbine effects cancel out each other. The overall effect of the upstroke in the thrust direction is thus equal to zero.
- Diagram 3
- A special lift distribution at the upstroke when the stroke momentum of the inner and outer wing section balanced each other exactly. Thus, the wing can be moved upwards without an external force.
Due to the lever action of the wing at this upstroke setting the positive lift close to the fuselage must be bigger than the negative lift at the wing tip. In total, there still remains some positive upstroke lift ( Otto Lilienthal 1889). The wing downstroke with its generally strong generation of lift and thrust can ensure the balance of the remaining forces during the whole flapping cycle.
Would one do without lift in favour of thrust generation in the upstroke the following should be considered. To generate the complete lift-pulse only in the downstroke - in virtually half of the available time - the lift force and consequently the wing area, too, would have to be almost doubled. This and the corresponding lift fluctuations are only appropriate in exceptions.
As to be seen in the diagram 1 shown lift distributions the average lift of both working cycles are different in size. At least at low flapping frequency, this will result in an obvious pendulous motion of the fuselage. But due to thereby generated variations of the angle of incidence it deadens itself quite effectively. These variations are not included in the diagrams.
Naturally, other settings are possible in the area close to the preceding lift distribution. They are well suited for gently inclined climb flights with a moderate flapping frequency. My EV-ornithopters have been built for this way of flying.
3.2 Cruising flight
Starting from the previously described flight scenario for the horizontal cruising flight it is more advantageous to increase the total lift during the upstroke and shift it a little more towards the wing tip. There, only a little bit of negative lift is generated - if any at all (please look at the force vectors of the following picture). But by this way, the wind turbine effect and its operating drag are increased.
That this should be beneficial is amazing at first. The wind turbine effect now can no longer be used for generating thrust in the area of the wing tip. Would it not be better simply to increase the flapping frequency?
- Forces at the wing of a stork
during up- and downstroke
by Otto Lilienthal
According to a proposal by Otto Lilienthal the wind turbine or the wing upstroke energy may also be used again in a 2nd possibility. At first, the operating drag slows down the flying ornithopter. Thereby detracted kinetic energy of the model can be accumulated in a spring. This spring must be positioned in a fashion that it is tensioned at the upstroke. It relaxes in the downstroke, supports thereby the flapping motion, generates thrust and transfers wing upstroke energy back to the kinetic energy of the model.
A 3rd possibility for using the wind turbine force lies in the acceleration of the wing mass in upstroke direction. If the wings are then slowed down at the upper final wing position by a spring and accelerated in downstroke direction, retransfer of the upstroke energy is also affected in this way. Thereby, the acceleration of the wing must not be limited to the initial stage of the upstroke.
In the upstroke, a mechanical drive of the flapping wing is not necessary in these cases. The wing even releases energy to the above-mentioned springs. Anyway, the wind turbine motion must act against any force. Otherwise no lift can be developed on a freely movable wing. The energy emitted during wing upstroke is normally relatively small. This is especially true when the lift is concentrated in the middle of the wing span.
A good way to decrease the wind turbine effect in spite of strong lift generation is the pulling or the dragging of the outboard wing section during the upstroke of the inboard wing section. Thereby the outboard section of the wing becomes an end plate or a winglet to the inboard section of the wing.
- This mainly has a bisecting effect on the effective wind turbine span.
- At the same time, it reduces with its winglet effect the induced drag of the inboard wing section.
- Furthermore, it reduces problems of wing inertia, particularly in the area of the upper final wing position.
To enable at the upstroke strong lift at the inboard wing section it will be equipped with large airfoil camber.
The flapping wing as an aerodynamic two-stroke machine constantly generates positive lift. In the direction of flight, however, it works with its thrust times forward (downstroke) and sometimes backward (upstroke). Nevertheless, together with the three possibilities mentioned above, the whole entire drive energy is used to generate thrust forward. Of course there are the usual losses due to the profile drag and the induced drag. However, this is always the case for the generation of lift.
In spite of changing acceleration direction, flight velocity should be kept constant. Thereby are definitely advantageous a high stroke frequency and a large model mass.
During such cruising flight configurations of the upstroke, its lift increase more than during the gently inclined flight. Apart from thrust generation also lift generation during downstroke can be released. Therefore, its lift distribution will be shifted rather towards the wing root and concurrently be adjusted smaller.
- Diagram 4
- Distributions of lift for a cruising flight with unlimited wingspan. Also the distribution of the upstroke is optimized in relation to the induced drag.
Altogether, in cruising flight the lift distributions of both of the work cycles have been approximated to those of gliding. One approximates them the more flow-favourable the aircraft is built. Less thrust is then necessary. Furthermore, the induced drag of the downstroke decreases noticeably this way.
Perhaps it might be enough to shift the lift only a little along the span, without changing its size - in the upstroke towards the wing root, in the downstroke towards the wing tip. However, a twisting of the wing root is necessary for that.
The advantage of the flapping wing working in the opposite
direction during upstroke and downstroke is the even generation of lift. Overall,
a very effective cruise flight can be achieved with thrust directed only forward
and not upward. This type of flight can also be named as
When this gait is perfected, it shows the following
characteristics according to
Konrad Lorenz (1933): A very slight bending
of the hand wing during upstroke and a constant lift. An up and down swinging
of the bird thereby is no longer observable (K. Lorenz named the flying with lift
glide rowing). The flapping frequency is significantly lower when flying
with lift than when flying with the following type of flight. The stroke frequency
is significantly lower when flying with lift than when in climb or hovering flight.
3.3 Strong inclined climb and hovering flight
Similar to a helicopter during flapping flight the weight force can be balanced
by a slipstream directed downward or by a thrust force directed upward. This is
Flying with thrust. Thereby, the wing upstroke practically
affected only with the drive. At least in steady flight, the thrust force is always
perpendicular to the wing-stroke plane and can be adjusted according to their
- Small bird on approach
If the thrust force points exactly in flight direction, there is either pure flying with thrust (perpendicular climb flight or hovering flight) or pure flying with lift (horizontal flight). In settings between these extremes and during a horizontal motion not too slow, the balance of all up weight is affected both by thrust and by lift directly generated at the wing. These mixed configurations are also assigned here to flying with thrust.
The taking off of an ornithopter, hovering on the spot, strong inclined climbing flight and slow horizontal flight are only possible according to the method flying with thrust.
In contrast, moderate fast horizontal flights can be conducted with both ways of flying - with quite a different demand for power, though. Relatively fast horizontal flights or cruising flight can be achieved only by flying with lift.
In flight praxis, especially the inclination of the stroke plane acts as identification criteria for ways of flying. In horizontal flight it is vertical to the flight direction. If it differs considerably (more than about 10 degrees) it is flying with thrust. Furthermore, a big upstroke wing twisting in a passive wing twisting is an indication for this way of flying - at least at high Reynolds numbers. Also, a relatively high power consumption relating to the horizontal velocity points to a flying with thrust.
Furthermore, the legs of birds, at least of the larger ones, are not fully stretched backwards when flying with thrust and their body still is not fully directed in flight direction ( R. Demoll 1930). But in publications of bird flight research it is only rarely pointed out to these both unequal ways of horizontal flight. The high power consumption during slow flight is commonly only ascribed to the thereby increasing induced drag (for an example please look at external link 2).
- A. Pénaud (1872)
Flying with thrust can be carried out in technical model making since the beginnings of aviation. But in horizontal flight of large and weightily ornithopters this way of flying demands considerably more energy than flying only with lift.
Otto Lilienthal had already distinguished clearly between these two ways of powered
flying among birds and has pointed out the enormous
flight energy during
4. How birds fly
Also birds apply the displacement of lift along the wing for propulsion or thrust generation. Erich v. Holst has illustrated it very clearly in the following scheme. In it, the location of the center of the lift distribution is represented by a wing section which is shiftable along the wing semi-span.
- Basic principle of lift and thrust
generation in the flight of birds
At the upper reversal point of the stroke motion it is shifted towards the wing tip and at the bottom point to the wing root. In this way, seen over a whole flapping period, while maintaining the normal force Q (or the lift) the thrust S gets larger than the backward directed force R.
With this ingenious trick of nature, it is possible to generate much lift also during the upstroke and nevertheless, seen over an entire stroke cycle, a thrust generation is made possible.
Because birds are shaped aerodynamically efficient it requires for them only a relatively small shifting of lift for the cruise flight (see, for example the position of the centers of pressure in diagram 4, above).
The physics of bird's flight, which is commonly used today, is based on an other idea. In it, in particular the arm wing is intended to generate lift during the up and downstroke. The thrust generated there during the downstroke is compensated by the back drive, generated there during the upstroke.
- Lift and thrust generation during a flapping period according to descriptions of the bird's flight with strong fluctuating lift.
- Supposedly approximate course of the lift distributions along the span according to the vague descriptions of the cruising flight of birds.
In the hand wing, a lot of thrust is been generated during the downstroke. During the upstroke, the hand wing is then guided upwards without any significant force, thus only with the remaining profile drag. It is said, that in this way the lift of the bird is mainly generated in the arm wing and the thrust in the hand wing. The large lift in the hand wing, which is necessary for generation of the large thrust during downstroke, is neglected in such a discription.
Sometimes, however, it is also said that during the downstroke the most lift arises (see the adjacent diagrams). About a rotation of the wing root during cruising flight of large birds, or other measures to increase lift during wing upstroke, is nothing reported. Thus, the lift changes considerably, seen over a whole flapping period.
Both bird flight theories, i.e. the common theory with strongly variable lift, and those with the shift of approximately constant lift, according to Erich von Holst, are in principle not so far apart. Both methods work with the displacement of lift - however with the birds it's not referred to as such. In both cases, the wing on upstroke can move upwards without drive, so only with the lift force.
If one compares in this context the calculated examples in the article Flapping wings with and without wing rotation (in German, PDF 0.7 MB) it can be seen that equable and uneven lift have preferences. This is also the case there because the size of the lift during wing upstroke is determined in particular by the choice of lift distribution. The flight mode with strongly changing lift offers advantages for gently inclined climb flight (see example 1, with c_Γ1=0) and the flight mode with relatively constant lift for long-distance flights (see example 10, with c_Γ1=5 or 6). But, again, the general rule applies: What is good for the lift, is bad for the thrust, and vice versa.
- Increased lift distribution on upstroke with the goal of a nearly constant lift during one stroke period
For ornithopters it is easier to realize the method with strong fluctuating lift,
as described in the commonly used physics of bird's flight. In this case you need
no rotation of the wing root. For long-distance flights, however, one should not
do without the advantages of an at least almost constant lift (please see also
Lift during wing upstroke,
version 10.0 , 2015 - 2018, PDF 0.9 MB).
Also in descriptions of the flight of birds the function of the wing downstroke is compared to a propeller. A corresponding analogy from wing upstroke with lift, with its well-known additional drag, cannot be found. The function as a wind turbine and its possibilities for using are obviously unknown. The physical cause of the additional drag, it's thrust against the flight direction, therefore remains in the dark. Also Otto Lilienthal and E. v. Holst mention this context only casually.
- Staggering of the primaries
of a stork during gliding
Professor Jeremy Rayner has researched the flight of birds at the University of
Leeds (England) and also already largely described the flight of birds with constant
circulation (see article
Vertebrate flapping flight mechanics and aerodynamics
and the Evolution of flight in bats in
Nachtigall W. 1986, BIONA-report 5).
He emphasizes the importance of this gait and sees its strong experimental confirmation
in the flow visualization experiments with a cestrel in fast flight by G. R. Speeding
(1982, The vortex wake of birds: an experimental investigation, Ph.D. Thesis,
University of Bristol, U.K.). They show a non-planar pair of vortices with variable
span, closely following the wings and missing approach vortices (please look at
external link 3 and the
Arrangements of wing tip vortices on flapping wings, PDF 0.5 MB).
A further clarification of the different theories of bird flight is possible in particular by measurements in the wind tunnel. Thereby the effects of various twists and rotations on the lift distributions along the span should to be measured on technical flapping wings. Further optimizations are possible by investigations on flapping wings with different contours as well as with and without bending of the hand wing. Also the behaviour of the tip vortices during twisting and rotation of the flapping wing is very informative.
Further details of the flapping wing theory and a calculation method that uses quasi-steady aerodynamics and blade element theory, which has already been used for flapping wings by Otto Lilienthal, can be found in the Handbook.