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| The '''elastic membrane analogy''', also known as the '''soap-film analogy''', was first published by pioneering aerodynamicist [[Ludwig Prandtl]] in 1903. | | The individual who wrote the article is known as Jayson Hirano and he completely digs that name. To play domino is some thing I really appreciate performing. Alaska is the only location I've been residing in but now I'm contemplating other options. Credit authorising is exactly where my main earnings arrives from.<br><br>my page online psychic readings - [http://cspl.postech.ac.kr/zboard/Membersonly/144571 no title] - |
| <ref>Prandtl, L.: "Zur torsion von prismatischen stäben", Phys. Zeitschr., '''4''', pp. 758-770 (1903)</ref>
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| <ref>Love 1944, article 224, page 322.</ref>
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| It describes the [[Stress (physics)|stress]] distribution on a long bar in [[torsion (mechanics)|torsion]]. The cross section of the bar is constant along its length, and need not be circular. The [[differential equation]] that governs the stress distribution on the bar in torsion is of the same form as the equation governing the shape of a membrane under differential pressure. Therefore, in order to discover the stress distribution on the bar, all one has to do is cut the shape of the cross section out of a piece of wood, cover it with a soap film, and apply a differential pressure across it. Then the slope of the soap film at any area of the cross section is directly proportional to the stress in the bar at the same point on its cross section.
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| ==Application to thin-walled, open cross sections==
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| While the membrane analogy allows the stress distribution on any cross section to be determined experimentally, it also allows the stress distribution on thin-walled, open cross sections to be determined by the same theoretical approach that describes the behavior of rectangular sections. Using the membrane analogy, any thin-walled cross section can be "stretched out" into a rectangle without affecting the stress distribution under torsion. The maximum shear stress, therefore, occurs at the edge of the midpoint of the stretched cross section, and is equal to <math>3T/bt^2</math>, where T is the [[torque]] applied, b is the length of the stretched cross section, and t is the thickness of the cross section.
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| It can be shown that the [[differential equation]] for the [[deflection surface]] of a homogeneous membrane, subjected to uniform lateral pressure and with uniform surface tension and with the same outline as that of the [[cross section (geometry)|cross section]] of a bar under [[Torsion (mechanics)|torsion]], has the same form as that governing the stress distribution over the cross section of a bar under [[Torsion (mechanics)|torsion]].
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| <!-- This equation is incorrect as it stands, so I am hiding it. | |
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| :<math>
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| \frac{p}{S} = 2G\frac{d\phi}{dz} = 2G\theta
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| </math> | |
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| -->
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| This analogy was originally proposed by [[Ludwig Prandtl]] in 1903.<ref>Prandtl, L.: "Zur torsion von prismatischen stäben", Phys. Z., '''4''', pp. 758-770 (1903).</ref>
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| ==Other applications==
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| Prandtl's stretched-membrane concept was used extensively in the field of electron tube ("vacuum tube") design (1930's to 1960's) to model the trajectory of electrons within a device. The model is constructed by uniformly stretching a thin rubber sheet over a frame, and deforming the sheet upwards with physical models of electrodes, impressed into the sheet from below. The entire assembly is tilted, and steel balls (as electron analogs) rolled down the assembly and the trajectories noted. The curved surface surrounding the "electrodes" represents the complex increase in field strength as the electron-analog approaches the "electrode"; the upward distortion in the sheet is a close analogy to field strength.
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| ==References==
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| {{Reflist}}
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| *{{cite book | last = Bruhn | first = Elmer Franklin
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| | title = ''Analysis and Design of Flight Vehicle Structures
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| | publisher = Jacobs Publishing | year = 1973 | location = Indianapolis
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| | pages = | url = | isbn = 0-9615234-0-9 }}
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| *{{cite book | last = Love | first = A. E. H.
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| | authorlink = Augustus Edward Hough Love
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| | title = A Treatise on the Mathematical Theory of Elasticity
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| | publisher = Dover | year = 1944 | location = New York
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| | pages = | url =
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| | isbn = 0-486-60174-9}}. Especially Chapter XIV, articles 215 through 224. "This Dover edition, first published in 1944, is an unaltered and unabridged republication of the fourth (1927) edition."
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| *{{cite book | last = | first =
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| | title = ''Advances in Electronics Volume 2
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| | publisher = | year = 1950 | location =
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| | pages = 141 | url = http://www.scribd.com/doc/73164400/26/IV-AUTOMATIC-TRAJECTORY-TRACING | isbn = }}
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| {{DEFAULTSORT:Membrane Analogy}}
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| [[Category:Mechanics]]
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| [[Category:Solid mechanics]]
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| [[Category:Structural analysis]]
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| [[Category:Analogy]]
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