n5312_s4b.doc
TRANSCRIPT
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ENG5312 Mechanics of Solids II
Discontinuity Functions
Discontinuity functions are used to develop a single epression for the
elastic curve of a !ultiply loaded "ea! or shaft#
$se of a single epression %ill per!it evaluation of integration constants
fro! "oundary conditions only& as continuity conditions %ill "e satisfiedauto!atically#
Define the Macaulay function:
x a n
= 0
(x a)n,x < a
,x a
%here n 0
'nd
x a n
dx = x a
n+1
n +1+ c
(his function can "e used to represent a unifor!ly distri"uted load& wo &
starting at x = a )
w(x) = wo
x a 0
i#e# w(x)= 0 for x
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ENG5312 Mechanics of Solids II
V(x) = wo x a =
0
wo(x a)
,x
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ENG5312 Mechanics of Solids II
So shear force and "ending !o!ent are given "y)
V(x) = w(x)dx= P x a 0
M(x)= V(x)dx= P x a 1
' !o!ent& M o& positive counter/cloc%ise& is a li!it as 0of theapplication of t%o distri"uted loads#
w(x) = Mo x a
2=
0
Mo
,x a
,x =a
.here the /2 eponent is used to guarantee the units of w(x) areforce0length#
(he shear force and "ending !o!ent that result fro! this epression are)
V(x) = w(x)dx = Mo x a
1
M(x) = V(x)dx = Mo x a
0
.here the integrals are perfor!ed using operational calculus#
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ENG5312 Mechanics of Solids II
(he functions used for the different loadings are su!!aried in (a"le 12/2
of 4i""eler#
(he discontinuity functions provide a !eans of directly specifying the
"ending !o!ent as a function for a "ea!# (his function can then "eintegrated to deter!ine the deflection& and only t%o "oundary conditions%ill "e reuired to evaluate the constants of integration#
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