Double Integration Method | Beam Deflections

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.
 

In calculus, the radius of curvature of a curve y = f(x) is given by
 

$\rho = \dfrac{[\,1 + (dy / dx)^2\,]^{3/2}}{\vert \, d^2y/dx^2 \, \vert}$
 

In the derivation of flexure formula, the radius of curvature of a beam is given as
 

$\rho = \dfrac{EI}{M}$
 

Deflection of beams is so small, such that the slope of the elastic curve dy/dx is very small, and squaring this expression the value becomes practically negligible, hence
 

$\rho = \dfrac{1}{d^2y/dx^2} = \dfrac{1}{y''}$
 

Thus, EI / M = 1 / y''
 

$y'' = \dfrac{M}{EI} = \dfrac{1}{EI}M$
 

If EI is constant, the equation may be written as:
 

where x and y are the coordinates shown in the figure of the elastic curve of the beam under load, y is the deflection of the beam at any distance x. E is the modulus of elasticity of the beam, I represent the moment of inertia about the neutral axis, and M represents the bending moment at a distance x from the end of the beam. The product EI is called the flexural rigidity of the beam.
 

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.