Aircraft structures for engineering students - part 5 pps

Aircraft structures for engineering students - part 5 pps

Aircraft structures for engineering students - part 5 pps

... Thus 4 .5 g mla =-3 g= 13.5kN Resolving forces parallel to the axis of the fuselage N - T + mlacos 10" - 4 .5 sin 10" = 0 N- 137.1 + 13 .5~ 0~10 ~-4 .5sin1O0=O 1.e. 4 .5 kN ... substituting for r(ue) from Eq. (8 .51 ) 3.23 1 05~ ;5. ’6 E(ue) = 1000/~0 Equation (8 .54 ) then becomes ) dtle D, = - 1; ( g)2 ( Su,e 7 SA :-)...
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Aircraft structures for engineering students - part 1 pps

Aircraft structures for engineering students - part 1 pps

... directions for each combination. a, N/m2 ay N/m2 7.u N/m2 (i) +54 +30 +5 (ii) +30 +54 -5 (iii) -6 0 -3 6 +5 (iv) +30 -5 0 +30 Am. (i) aI = +55 N/mm2, arI = +29N/mm2, a1 at 11 .5& quot; ... load for a flat plate 51 51 59 61 63 65 65 68 68 70 71 73 76 77 85 100 103 103 107 109 110 110 122 122 1 25 129 137 141 14...
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Aircraft structures for engineering students - part 9 pps

Aircraft structures for engineering students - part 9 pps

... matrix for a uniform beam 51 1 It is possible to write Eq. (12.44) in an alternative form such that the elements of [KJ are pure numbers. Thus 12 -6 -1 2 -6 -6 4 62 -1 2 6 12 6 -6 2 64 This form ... Stiffness matrix for a uniform beam 51 5 The beam may be idealized into two beam-elements, 1-2 and 2-3 . From Fig. 12.11 we see that v1 = v3 = 0,...
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Aircraft structures for engineering students - part 2 pot

Aircraft structures for engineering students - part 2 pot

... BC 3000 R 1 DA 3000 R 1 AC 50 00 -5 R/3 -5 13 1 25 000R/9 8 75 DB 50 00 -5 R/3 -5 13 1 25 000R/9 8 75 C = 48 OOOR Problems 67 Fig. P.3 .5 P.3 .5 Determine the maximum shear stress ... M = - (L - z) - -Rz, hence - = - -2 and between B and C P fi dM d3 4 2 dR 2 M =-( L-z) R(L-z), hence -= (L-z) Thus...
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Aircraft structures for engineering students - part 3 docx

Aircraft structures for engineering students - part 3 docx

... zero then d2W - a2W d2W - d2W ax2 - 8Y2 ay2 - dX2 - -v- or - -v- and the plate has curvatures of opposite signs. The case of My = 0 is illustrated in Fig. 5. 3. A surface ... q(x,y)sin-sin- dxdy . mrx m'rx nry n'ry sin - sin - dx dy = m=l 2 n=l T/:jIamsin-sin- a a b b - ab 4 - since a 2 _- - wh...
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Aircraft structures for engineering students - part 4 docx

Aircraft structures for engineering students - part 4 docx

... 5 one simply supported 0 1 2 3 4 I5 I3 II 9- 7- 5, k - - - a/b (b) k 4 0- 36 - Clamped edges Simply supported 123 45 a/b (C) Fig. 6.16 (a) Buckling coefficients for ... Flexural-torsional buckling of thin-walled columns 1 85 0 P - ~EIJL~ -Pxs P - ~EI,,JL~ 0 PYS PYS - Pxs IOPIA - .rr2ET/L2 - GJ =O...
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Aircraft structures for engineering students - part 6 potx

Aircraft structures for engineering students - part 6 potx

... = 25mm of 4.3 N/mm. In the wall 23 q23 = -6 9.0 x 1 0-~ 2 x 75ds2 - 34 .5 r i.e. q23 = -1 .04,~2 - 34 .5 Hence q23 varies linearly from a value of -3 4 .5 N/mm at 2 to -1 38 .5 N/mm ... right-hand side of Eq. (ii) we have r=l qb:23 = qb,34 = -7 .22 X 1 0-4 (400 X 100) = -2 8.9N/mm qb,4j = -2 8.9 - 7.22 x io-4(ioo x...
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Aircraft structures for engineering students - part 7 ppt

Aircraft structures for engineering students - part 7 ppt

... qb:27 = -1 .07 x qb,J6 = -1 .07 x x 3880 x 230 = -9 5. 5N/mm x 258 0 x 1 65 = -4 5. 5N/mm qb $5 -4 5. 5 - 1.07 x io-4 x 258 0 x (-1 65) = 0 qb .57 = 1.07 X qb;38 = -1 .07 ... For cell I For cell I1 [-2 50 qI + qII( 250 + 7 25 + 233 + 7 25) - 233q11~] (ii) de 1 dz - 2 x 355 OOOGREF _- F...
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Aircraft structures for engineering students - part 8 doc

Aircraft structures for engineering students - part 8 doc

... 12, 56 51 0 0 .55 9 1,6 6 45 I 93 000 23, 45 1 65 0.9 15 2, 5 1290 I1 258 000 34: 10 15 0 .55 9 3,4 19 35 38 304 2.030 25 304 1.6 25 Ans. 241.4mm. P.10.13 A portion of a tapered, three-cell ... substitute in Eq. (1 1.28) for q from Eq. (1 1. 25) and for PB from Eq. (1 1.26). Hence 1 #PA - Gt ( PA S,Z PA) - - - - -...
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Aircraft structures for engineering students - part 10 pot

Aircraft structures for engineering students - part 10 pot

... aeroelasticity For a non-trivial solution (1 - 16d) -1 5Xw’ -( 1 - 6XJ) Expanding this determinant we have or -( 1 - 16Xw2)(1 - 6XJ) + 75( Xw2)’ = 0 21(AJ)’ - 22xw2 + 1 = ... the form shown in Fig. 13.10. Substituting the second natural frequency in Eq. (vii) we have - - ~2 1 - 16Xw2 - 1 - 16 x (1/21) 15 -...
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