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Beam with two symmetrical loads by moment-area

Short answer

Slope at supports = Pa(L–a)/(2EI); mid-span deflection = Pa(3L²–4a²)/(24EI). For L=6 m, a=2 m, P=30 kN, EI=25000 kN·m²: slopes = 4.8×10⁻³ rad, maximum deflection = 9.2 mm downward.

A simply supported beam of span L carries two equal point loads P, each at a distance a from the nearer support. Using the moment-area method, derive expressions for the slope at the supports and the deflection at mid-span. Evaluate them for L = 6 m, a = 2 m, P = 30 kN and EI = 25 000 kN m^2.

Set-up

    P            P
    |            |
    v____________v
  A   a   |  L-2a   a  B
 R_A = P   R_B = P

By symmetry RA=RB=PR_A = R_B = P. Bending moment: rises linearly from 0 at A to PaPa at the load, then constant PaPa between the loads. The M/EIM/EI diagram is a trapezoid, symmetrical about mid-span C.

Slope at support A

By symmetry the slope at mid-span C is zero (the tangent at C is horizontal). By Theorem I, the slope at A equals the area of the M/EIM/EI diagram between A and C:

θA=1EI[12 a (Pa)+(L2−a)(Pa)]=Pa(L−a)2EI\theta_A = \frac1{EI}\left[\frac12\,a\,(Pa) + \left(\frac L2-a\right)(Pa)\right] = \frac{Pa(L-a)}{2EI}

Deflection at mid-span

The deflection at C equals the deviation of A from the tangent at C, i.e. the moment of the area between A and C about A (Theorem II):

yC=1EI[Pa22⋅2a3+Pa(L2−a)(L4+a2)]y_C = \frac{1}{EI}\left[\frac{Pa^2}{2}\cdot\frac{2a}{3} + Pa\left(\frac L2-a\right)\left(\frac{L}{4}+\frac a2\right)\right]

The first term is the triangle (centroid 2a/32a/3 from A); the second is the rectangle (centroid at a+12(L2−a)=L4+a2a + \frac12(\frac L2 - a) = \frac L4+\frac a2).

yC=1EI[Pa33+PaL28−Pa32]=Pa (3L2−4a2)24EIy_C = \frac{1}{EI}\left[\frac{Pa^3}{3} + \frac{PaL^2}{8} - \frac{Pa^3}{2}\right] = \boxed{\frac{Pa\,(3L^2-4a^2)}{24EI}}

Numerical values

θA=30×2×(6−2)2×25000=4.8×10−3 rad\theta_A = \frac{30\times2\times(6-2)}{2\times25000} = 4.8\times10^{-3}\ \text{rad} yC=30×2×(3×36−4×4)24×25000=60×92600000=9.2×10−3 my_C = \frac{30\times2\times(3\times36-4\times4)}{24\times25000} = \frac{60\times92}{600000} = 9.2\times10^{-3}\ \text{m}

Answer: θA=θB=4.8×10−3\theta_A = \theta_B = 4.8\times10^{-3} rad (0.275∘)(0.275^\circ); maximum deflection at mid-span =9.2= 9.2 mm downward.

✓ Answer checked by Claude Opus 5.5 (high effort)

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