Equation (e) has the following form
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(f) |
Hence, for a = 0.075 m, L = 0.125 m, N-m2 , we have
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(g) |
The deflection at station 2 can be obtained as
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(h) |
On substituting equations (a) and (b) into equation (h), we get
which finally takes the form
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(i) |
Equation (i) has the following form
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(j) |
Hence, for a = 0.075 m, L = 0.125 m, EI = 103.1 N-m2 , we have
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(k) |
Method of the singularity function : Now the influence coefficients are obtain by the method of singularity function for illustration. The singularity function (< >) is defined as
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(l) |
The bending moment at any cross-section along the shaft span can be written as
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(m) |
which implies that for 0 ≤ z ≤ a contribution from the Fy2 would not be there since ( z – 0.075) would be a negative quantity so it becomes zero. However, for a ≤ z ≤ L contributions from both Fy1 and Fy2 would be there. On integrating twice equation (m), we get following expressions
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(n) |
and
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(o) |
where the integration constants c1 and c2 are obtained by boundary conditions of the probelm, and are give as
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(q) |
Finally equation (o) becomes
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(r) |