Biyernes, Abril 01, 2011

Beam Defections: Double Integration Method

The double integration method is a powerful tool in solving deflection and slope of a beam at any point because we will be able to get the equation of the elastic curve.


For a beam with flexural rigidity EI constant, the differential equation is given by
$ \dfrac{d^2y}{dx^2} = \dfrac{M}{EI} $

Where y represents the vertical deflection; M is the bending moment at a distance x from the conveniently selected origin; E is the modulus of elasticity or Young's modulus; I is the moment of inertia of the beam section; and the product EI is called the flexural rigidity.
Integrating the above equation once will give us dy/dx which is the equation of the slope of elastic curve, usually denoted by ?. Integrating once more (thus, double integration) will result to y which is the equation of the deflection. We can write it into symbols as follows
$ \dfrac{dy}{dx} = \theta = \displaystyle \int \dfrac{M}{EI} + C_1 $
and
$ \displaystyle y = \int \int \dfrac{M}{EI} + C_1x + C_2 $
The constants of integration C1 and C2 can be found by applying appropriate boundary conditions.

The first integration y' yields the slope of the elastic curve and the second integration y gives the deflection of the beam at any distance x. The resulting solution must contain two constants of integration since EI y" = M is of second order. These two constants must be evaluated from known conditions concerning the slope deflection at certain points of the beam. For instance, in the case of a simply supported beam with rigid supports, at x = 0 and x = L, the deflection y = 0, and in locating the point of maximum deflection, we simply set the slope of the elastic curve y' to zero.

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