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Hardcover Aircraft Structures Book

ISBN: 0070491968

ISBN13: 9780070491960

Aircraft Structures

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Still relevant decades after its 1950 publication, this legendary reference text on aircraft stress analysis is considered the best book on the subject. It emphasizes basic structural theory, which... This description may be from another edition of this product.

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David J. Peery, "Aircraft Structures"

David J. Perry's "Aircraft Structures" is indisputably a classic reference for the students and practicing engineers as well, and most likely a best text book ever written on the subject of the static strength and stability of metallic aircraft structures and its components. However, both editions, the original from 1950, and 2nd from 1982, contain a minor error in "Joints and Fittings" Chapter (page 304 of 1950 edition, page 397 of 2nd edition): The last paragraph contains a statement: " ... in Fig. 12.15.(c), which yields maximum bearing stresses, 4P/tb at the inside corner and 2P/tb at the outside corners." Conversely, these bearing stress expressions don't agree with those (i.e., 4P/td, 2P/td) shown in Fig. 12.15.(c). Because the text doesn't corroborate how it was arrived to the maximum pin bending moment 4Pt/27 [InLb] shown on page 305, this discrepancy may confuse the issue. That this indeed may lead to the confusion is evident in Michael Niu's "Airframe Stress Analysis and Sizing", 2nd edition, page 275, Eq. 9.1.1. Here in all likelihood Niu copied Peery's equation (12.8), but apparently unable to reconcile mentioned discrepancies, in the equation simply left out plate width "b", and not addressing the maximum bearing stress in question, boldly claims that this tensile stress is for "1.0 inch - wide strap". In the equation (12.8) Peery logically concludes, that if the axial stresses (as derived from the equation P/A ± M/W at both plate faces) are four times (resp. two times) of the average stress value, then same should be valid for the pin bearing stresses too. In other words, at a point, the load intensity (unit loading) producing maximum axial stress in the plate has to be equal to the load intensity causing the maximum bearing stress on the pin. This means, that the extreme load intensities on the pin will be obtained by dividing extreme plate stresses by plate width "b". Then by dividing these extreme load intensities by the pin diameter, one will obtain pin bearing stresses at both plate faces, and these expressions are in agreement with those shown in Fig. 12.15.(c). And thus the text in last paragraph on this page should read: "...,which yields maximum bearing stresses, 4P/td at the inside corner and 2P/td at the outside corners ...". If one constructs shear force diagram, then at the outside of the plate the pin shear force equals to 0 [Lb], at 1/3t (measured from outside of the plate) the shear force equals to P/3 [Lb] , at 2/3t (measured from plate outside) the shear force equals to 0 [Lb] (i.e., the location of maximum bending moment), and on the inside of the plate the shear force has to balance with the applied load P [Lb]. For the moment diagram, the pin bending moments equal to zero at both plate faces, and the maximum moment, Mmax = 2 x (P/3 x 2/3 x t/3) = 4Pt/27 [InLb] exists in the location where the internal shear force in the pin changes its sign, i.e. at t/3 measured from the inside of the plate. Perry's "Aircr

An essential and readable introduction to aircraft structure

This is an update of a classic and excellent textbook on aircraft structures. I recommend it highly.
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