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Conjugate beam: overhanging beam free end

Short answer

By the conjugate beam method, the conjugate beam has hinges at A and C and a fixed end at the overhang tip. The free end D deflects upward by 1100/EI and rotates 450/EI anticlockwise.

Determine deflection and rotation at free end of the overhanging beam shown in figure below. Use conjugate beam method. [Figure: beam ABCD; A hinge, C roller; AB = 6 m and BC = 6 m with flexural rigidity 2EI and 300 kN at B; overhang CD = 2 m (EI) with 150 kN at D.]

Given data

Beam ABCD: A hinge at 0, B at 6 m (300 kN), C roller at 12 m, D free end at 14 m with 150 kN. ACAC (=12= 12 m) has 2EI2EI; overhang CD=2CD = 2 m has EIEI.

      300 kN                          150 kN
 A ------v------------------ C --------v D
 ^   6 m B      6 m   (2EI)  ^  2 m (EI)

Step 1: Reactions

RA=125.00R_{A} = 125.00 kN, RC=325.00R_{C} = 325.00 kN (positive = upward; check: ∑Fy=450.00\sum F_y = 450.00 kN equals the total load 450.00 kN).

Step 2: Bending moment diagram (sagging +), as M/EIM/EI pieces

Portion (m)MM (kNm)stiffnessArea of M/EIM/EIxˉ\bar x from A (m)
0 to 6125x125 x2EI1125.004.000
6 to 121800−175x1800 - 175 x2EI675.006.667
12 to 14150x−2100150 x - 2100EI-300.0012.667

(Stiffness is in terms of EIEI; "Area" is ∫M/EI dx\int M/EI\,dx in units of 1/EI1/EI; xˉ\bar x is the centroid distance from A.)

Step 3: Conjugate beam

The real beam has a hinge at A, a roller at the second support and a free end at the overhang tip, so the conjugate beam has a hinge at A, an internal hinge at the support and a fixed end at the tip. It carries the M/EIM/EI diagram of Step 2 as load (sagging M/EIM/EI acts downward, hogging acts upward). Conjugate shear V′V' = slope (positive = clockwise) and conjugate moment M′M' = deflection (positive = downward).

Step 4: Conjugate reaction at A (slope at A)

Taking moments of the conjugate beam about the support at x=12x = 12 m (conjugate moment is zero there):

RA′×12=(1125.00)(8.000)+(675.00)(5.333)=12600.00R'_A\times12 = (1125.00)(8.000) + (675.00)(5.333) = 12600.00 RA′=1050.000EI (slope at A, clockwise)R'_A = \frac{1050.000}{EI}\ \text{(slope at A, clockwise)}

At B (300 kN) (x=6x = 6 m):

V′=RA′−∑A=1050.000−[(1125.00)]=−75.000EI (slope, anticlockwise)V' = R'_A - \sum A = 1050.000 - [(1125.00)] = \frac{-75.000}{EI}\ \text{(slope, anticlockwise)} M′=RA′ x−∑A(x−xˉ)=6300.000−[(1125.00)(2.000)]=4050.000EI (deflection, downward)M' = R'_A\,x - \sum A(x-\bar x) = 6300.000 - [(1125.00)(2.000)] = \frac{4050.000}{EI}\ \text{(deflection, downward)}

At D (free end) (x=14x = 14 m):

V′=RA′−∑A=1050.000−[(1125.00)+(675.00)+(−300.00)]=−450.000EI (slope, anticlockwise)V' = R'_A - \sum A = 1050.000 - [(1125.00) + (675.00) + (-300.00)] = \frac{-450.000}{EI}\ \text{(slope, anticlockwise)} M′=RA′ x−∑A(x−xˉ)=14700.000−[(1125.00)(10.000)+(675.00)(7.333)+(−300.00)(1.333)]=−1100.000EI (deflection, upward)M' = R'_A\,x - \sum A(x-\bar x) = 14700.000 - [(1125.00)(10.000) + (675.00)(7.333) + (-300.00)(1.333)] = \frac{-1100.000}{EI}\ \text{(deflection, upward)}

Answer: at the free end D the deflection is 1100EI\dfrac{1100}{EI} upward (the 150 kN load is small compared with the span load, so the overhang rises), and the rotation is 450EI\dfrac{450}{EI} anticlockwise (kNm3^3/EI and kNm2^2/EI).

✓ Answer checked by Claude Opus 5.5 (high effort)

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