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Vibrations of Shells and Plates, Third Edition

With more and more subtle buildings excited by glossy engineering, wisdom of the complicated vibration habit of plates, shells, curved membranes, jewelry, and different complicated buildings is key for today’s engineering scholars, because the habit is essentially diversified than that of easy constructions equivalent to rods and beams.

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Let is and js , 1 ≤ s ≤ r, r ≤ n, denote r integers such that 1 ≤ i1 < i2 < · · · < ir ≤ n, 1 ≤ j1 < j2 < · · · < jr ≤ n and let n xi = aij ek , 1 ≤ i ≤ n, k=1 r yi = aijt ejt , 1 ≤ i ≤ n, t=1 zi = xi − yi . Then, any vector product is which the number of y’s is greater than r or the number of z’s is greater than (n − r) is zero. ir where the vector product on the right is obtained from (z1 · · · zn ) by replacing zis by yis , 1 ≤ s ≤ r, and the sum extends over all nr combinations of the numbers 1, 2, .

B2n ... . . bnn . 15) 2n Reduce all the elements in the first n rows and the first n columns, at present occupied by the aij , to zero by means of the row operations n Ri = Ri + aij Rn+j , j=1 1 ≤ i ≤ n. 16) 34 3. Intermediate Determinant Theory The result is: c11 c21 ... cn1 An Bn = −1 b11 −1 b21 ... −1 bn1 c12 c22 ... cn2 b12 b22 ... bn2 . . c1n . . c2n ... . . cnn . . b1n . . b2n ... . . bnn . 17) 2n The product formula follows by means of a Laplace expansion. cij is most easily remembered as a scalar product:   b1j b  cij = ai1 ai2 · · · ain •  2j  .

B1n . . b2n ... . . bnn . 17) 2n The product formula follows by means of a Laplace expansion. cij is most easily remembered as a scalar product:   b1j b  cij = ai1 ai2 · · · ain •  2j  . 18) ··· bnj Let Ri denote the ith row of An and let Cj denote the jth column of Bn . Then, cij = Ri • Cj . Hence An Bn = |Ri • Cj |n R1 • C1 R1 • C2 R2 • C1 R2 • C2 = ······ ······ Rn • C1 Rn • C2 · · · R1 • Cn · · · R2 • Cn ··· ······ · · · Rn • Cn . 19) n Exercise. If An = |aij |n , Bn = |bij |n , and Cn = |cij |n , prove that An Bn Cn = |dij |n , where n n dij = air brs csj .

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