FIGURE 39
section; wx = load intensity at the given section; M and m = bending moment at the given
section induced by the actual load and by the unit moment, respectively.
- Evaluate the moments in step 1
Evaluate M and m. By proportion, Wx = w(L - x)/L; M = -(x^2 /6)(2w + wj = -(wx^2 /6)[2 +
(L - x)IL\ = -wx^2 (3L - x)/(6L); m = -. - Apply a suitable slope equation
Use the equation (^0) A = /§ [MmI(EI)] dx. Then ElBA = So [^x^2 3L - x)l(6L)] dx = [w/(6L)]
x/£ (ILx^2 - jc^3 ) dx = [wl'(6L)](SLx^3 /3 - *^4 /4)]£ = [w/(6L)](L^4 - L^4 /4); thus, ^ - %wL^3 /
(EI) counterclockwise. This is the slope at A.
- Apply a unit load to the beam
Apply a unit downward load at A as shown in Fig. 39c. Let m' denote the bending mo-
ment at a given section induced by the unit load. - Evaluate the bending moment induced by the unit load;
find the deflection
Apply yA = So [Mm'I(EI)] dx. Then m' =-x; EIyA = /§ [wx\3L - x)l(6L)] dx = [w/(6L)]
x/J x\3L -x) dx;yA = (1 l/120)wZ^4 /(£7).
The first equation in step 3 is a statement of the work performed by the unit moment at
A as the beam deflects under the applied load. The left-hand side of this equation express-
es the external work, and the right-hand side expresses the internal work. These work
equations constitute a simple proof of Maxwell's theorem of reciprocal deflections, which
is presented in a later calculation procedure.
DEFLECTION OFA CANTILEVER FRAME
The prismatic rigid frame ABCD (Fig. 4Oa) carries a vertical load P at the free end. Deter-
mine the horizontal displacement of A by means of both the unit-load method and the mo-
ment-area method.
( b) Superimposed moment to find (^0) A
( Q) Actual load on beam