Beam Deflections - Triangular Load first created 07/05/07 - last modified 11/05/07 Page Author: Ty Harness
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Figure 1 - Encastre beam with a triangular load


From figure 1 we can see the load q is distributed as a triangle above the beam and using the equation of a straight line:

$q(x) = 2/L*q_0 *x$ for $0 < x < L/2$ .....(1)

Neglecting the beams self weight and assuming the reactions Ra and b are equal then using the equations of statics we can say :

$2*R_a = (q_0/2)*L$ .....(2)

$R_a = (q_0*L)/4$ .....(3)

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Figure 2 - Slicing the beam and adding a shear force V and Moment to ensure beam is still in equilibrium


Slicing the beam at x we can write down the bending moment equation to the left of x where the shearing force V will cause no moment:

$M = (q_0*L)/4*x - 1/2*q*x *(x/3) - M_a$ .....(4)

where x/3 is the centroid of the load triangle taken from x. Noting the problem is statically indeterminate we can't find Ma from the equations of statics alone and we'll need to use boundary conditions.

Substituting q from equation 1 into equation 5 and simplifying:

$M = (q_0*L*x)/4 - (q_0 *x^3)/(3*L) - M_a$ .....(5)

Using the general beam bending equation

$EI*(d^2y)/dx^2 = M = (q_0*L*x)/4 - (q_0 *x^3)/(3*L) - M_a $ .....(6)

Integrating with respect to x where A is a constant of integration:

$EI*dy/dx = (q_0*L*x^2)/8 - (q_0 *x^4)/(12*L) - M_a*x + A $ .....(7)

We know with the clamped beam of figure 2 that the slope when x=0 is zero:

$ 0 = (q_0*L*x^2)/8 - (q_0 *x^4)/(12*L) - M_a*x + A $ .....(8)

and that would mean A = 0. As mentioned, we need another boundary condition to find Ma and the symmetrical nature of the problem we could assume the slope at L/2 is also zero which is just still valid for the derived bending moment equation.

$ 0 = (q_0*L*(L/2)^2)/8 - (q_0 *(L/2)^4)/(12*L) - M_a*(L/2) $ .....(9)

which should simplify to

$M_a = 5/96*q_0*L^2$ .....(10)

Integrating the slope equation with respect to x and again B is a constant of integration:

$EI*y = (q_0*L*x^3)/24 - (q_0 *x^5)/(60*L) - 5/192*q_0*L^2*x^2 + B $ .....(11)

When x=0 then y=0 therefore from equation 11 then B must equal zero.

The deflection equation:

$EI*y = (q_0*L*x^3)/24 - (q_0 *x^5)/(60*L) - 5/192*q_0*L^2*x^2 $ .....(12)

The maximum deflection will be at L/2:

$E*I*y(L/2) = (q_0*L*(L/2)^3)/24 - (q_0 *(L/2)^5)/(60*L) - 5/192*q_0*L^2*(L/2)^2 $ .....(13)

$E*I*y(L/2) = -7/3840 * q_0 * L^4$ .....(14)


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