Lift-to-drag ratio
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2008-07-09T13:55:23Z
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In [[aerodynamics]], the '''lift-to-drag ratio''', or '''L/D ratio''' ("ell-over-dee" in the US, "ell-dee" in the UK), is the amount of [[Lift (force)|lift]] generated by a [[wing]] or vehicle, compared to the [[drag (physics)|drag]] it creates by moving through the air. A "better" L/D ratio is one of the major goals in wing design, since a particular aircraft's needed lift doesn't change, delivering that lift with lower drag leads directly to better fuel economy, climb performance and [[glide ratio]].
The term is calculated for any particular speed by measuring the lift generated, then dividing by the drag it causes. These vary with speed, so the results are typically plotted on a 2D graph. In almost all cases the graph forms a U-shape, due to the two main components of drag on the wing.
==Drag==
[[Induced drag]] is caused by the generation of lift by the wing. Lift generated by a wing is perpendicular to the wing, but since wings typically fly at some small [[angle of attack]], this means that a component of the force is directed to the rear. The rearward component of this force is seen as drag. At low speeds an aircraft has to generate lift with a higher angle of attack, thereby leading to greater induced drag. This term dominates the low-speed side of the L/D graph, the left side of the U.
[[Profile drag]] is caused by air hitting the wing itself. This form of drag, simply another name for [[wind resistance]], varies with the square of speed (see [[drag equation]]). For this reason profile drag is only a real factor at higher speeds, forming the right side of the L/D graph's U shape. Profile drag is lowered primarily by using thinner wings, but such a shape often leads to less low-speed lift, and thus higher induced drag.
[[image:Drag_Curve_2.jpg|thumb|right|The drag curve]]
It is the bottom point of the graph, the point where the combined drag is at its lowest, that the wing is performing at its best. For this reason designers will typically select a wing with its L/D peak at the chosen cruising speed of the aircraft, thereby maximizing economy. Like all things in [[aeronautical engineering]], the lift-to-drag ratio is not the only consideration for wing design. Performance at high [[angle of attack]] and a gentle [[Stall (flight)|stall]] are often considered more important, and for this reason easy-to-fly wing designs like the [[Clark-Y]] continue to be used even though many more efficient wings have since been designed.
==Glide ratio==
As the aircraft [[fuselage]] and control surfaces will also add drag and possibly some lift, it is fair to consider the L/D of the aircraft as a whole. As it turns out, the [[glide ratio]], which is the ratio of an (unpowered) aircraft's descent to its forward motion, is numerically equal to the aircraft's L/D. This is especially of interest in the design and operation of high performance [[gliders]] (called [[sailplanes]]), which can have glide ratios approaching 60 to 1 (60 units of distance forward for each unit of descent) in the best cases, but with 30:1 being considered good performance for general recreational use. Achieving a sailplane's best L/D in practice requires precise control of airspeed and smooth and restrained operation of the controls to reduce drag from deflected control surfaces. In zero wind conditions, L/D will equal altitude lost divided by distance traveled. Achieving the maximum distance for altitude lost in wind conditions requires further modification of the best airspeed, as does alternating cruising and thermaling. To achieve high speed across country, gliders are often loaded with water ballast to increase the airspeed (allowing better penetration against a headwind). As noted below, to first order the L/D is not dependent on speed, although the faster speed means the airplane will fly at higher [[Reynold's number]].
==Maximum range==
For maximum [[Range (aircraft)|range]], one should fly at the point on the graph with minimum drag. Since the lift on an aircraft must equal the weight, this point is equal to the maximum L/D point. (The speed should decrease a bit during the flight because the optimal speed decreases as the plane uses up fuel and becomes lighter.)
Because this theoretical speed may still be slightly exceeded without significant losses in efficiency, the "long range cruise speed" is normally slightly higher than the maximum range speed. There is a trade-off between saving fuel and saving time. The upper limit of speed is dictated by available (continuous) thrust and is not shown on the graph.
==Theory==
Mathematically, the maximum lift-to-drag ratio can be estimated as:
<math>(L/D)_{max} = \frac{1}{2} \sqrt{\frac{\pi A \epsilon}{C_{D,0}}}</math><ref>{{cite web|author=Loftin, LK, Jr.|title=Quest for performance: The evolution of modern aircraft. NASA SP-468|url=http://www.hq.nasa.gov/pao/History/SP-468/cover.htm|accessdate=2006-04-22}}</ref>,
where ''A'' is the [[aspect ratio (wing)|aspect ratio]], <math>\epsilon</math> is the aircraft's efficiency factor, and <math>C_{D,0}</math> is the [[zero-lift drag coefficient]].
==Supersonic/hypersonic lift to drag ratios==
At very high speeds, lift to drag ratios tend to be lower. [[Concorde]] had a lift/drag ratio of around 7 at Mach 2, whereas a 747 is around 17 at about mach 0.85.
[[Dietrich Küchemann]] developed an empirical relationship for predicting L/D ratio for high Mach:<ref>[http://www.aerospaceweb.org/design/waverider/design.shtml Aerospaceweb.org Hypersonic Vehicle Design]</ref>
<math>L/D_{max}=\frac{4(M+3)}{M}</math>
Windtunnel tests have shown this to be roughly accurate.
==Examples==
The following table includes some representative L/D ratios.
{| class="prettytable"
!Flight article
!Scenario
!L/D ratio
|-
!Modern Sailplane
|gliding
|~60
|-
![[Virgin Atlantic GlobalFlyer]]
|Cruise
|37<ref>David Noland, "Steve Fossett and Burt Rutan's Ultimate Solo: Behind the Scenes," ''Popular Mechanics'', Feb. 2005 ([http://www.popularmechanics.com/science/air_space/1262012.html?page=3 web version])</ref>
|-
![[Lockheed U-2]]
|Cruise
|~28
|-
![[Rutan Voyager]]
|Cruise<ref>David Noland, "Steve Fossett and Burt Rutan's Ultimate Solo: Behind the Scenes," ''Popular Mechanics'', Feb. 2005 ([http://www.popularmechanics.com/science/air_space/1262012.html?page=3 web version])</ref>
|27
|-
![[Albatross]]
|
|20<ref name=fili>[http://aerodyn.org/HighLift/ld-tables.html#table2 Fillipone]</ref>
|-
![[Boeing 747]]
|Cruise
|17
|-
![[Gimli glider]]
|Fuel exhaustion
|~12
|-
![[Common tern]]
|
|12<ref name=fili/>
|-
![[Herring gull]]
|
|10<ref name=fili/>
|-
![[Concorde]]
|M2 Cruise
|7.14
|-
![[Cessna 150]]
|Cruise
|7
|-
![[Concorde]]
|Approach
|4.35
|-
![[House sparrow]]
|
|4<ref name=fili/>
|-
![[Apollo Command/Service Module|Apollo CM]]
|Reentry
|0.368<ref>[http://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19690029435_1969029435.pdf Hillje, Ernest R., "Entry Aerodynamics at Lunar Return Conditions Obtained from the Flight of Apollo 4 (AS-501)," NASA TN D-5399, (1969).]</ref>
|}
==References==
<!--See http://en.wikipedia.org/wiki/Wikipedia:Footnotes for an explanation of how to generate footnotes using the <ref(erences/)> tags-->
<references/>
[[Category:Wing design]]
[[Category:Engineering ratios]]
[[Category:Aviation terminology]]
[[Category:Wind power]]
==See also==
*[[Specific fuel consumption]] the lift to drag determines the required thrust to maintain altitude (given the aircraft weight), and the SFC permits calculation of the fuel burn rate
*[[thrust to weight ratio]]
*[[Inductrack]] [[maglev]] has a higher lift/drag ratio than aircraft at sufficient speeds
*[[Gravity drag]] [[rocket]]s can have an effective lift to drag ratio while maintaining altitude
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