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Moment area: girder with 120 kN and 80 kN

Short answer

Moment area results: at 120 kN load, slope 0.00414 rad clockwise, deflection 15.64 mm down; at 80 kN load, slope 0.00282 rad anticlockwise, deflection 19.93 mm down. Maximum deflection 23.65 mm down at 6.87 m from left support.

A horizontal girder of steel having uniform section 14 m long is simply supported at its end. It carries concentrated loads of 120 kN and 80 kN at two points 3 m and 4.5 m from the two end supports respectively. Calculate the deflection and slopes of the girder at the point under the loads using moment area method. Take I=16×108 mm4I = 16\times10^8\ \text{mm}^4 and E=210 kN/mm2E = 210\ \text{kN/mm}^2. Verify the results using conjugate beam method. Also find magnitude and location of the maximum deflection in the beam.

Given data

Simply supported girder, span 14 m. 120 kN at 3 m from the left support A; 80 kN at 4.5 m from the right support B (i.e. 9.5 m from A). I=16×108I = 16\times10^8 mm4=1.6×10−3^4 = 1.6\times10^{-3} m4^4, E=210E = 210 kN/mm2=2.1×108^2 = 2.1\times10^8 kN/m2^2, so

EI=2.1×108×1.6×10−3=3.36×105 kNm2EI = 2.1\times10^8\times1.6\times10^{-3} = 3.36\times10^5\ \text{kNm}^2

Part 1: Moment-area method

Step 1: Reactions

RA=120.00R_{A} = 120.00 kN, RB=80.00R_{B} = 80.00 kN (positive = upward; check: ∑Fy=200.00\sum F_y = 200.00 kN equals the total load 200.00 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 3120x120 xEI540.002.000
3 to 9.5360360EI2340.006.250
9.5 to 141120−80x1120 - 80 xEI810.0011.000

(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: Tangent at A

Deviation of the support at x=14x = 14 m from the tangent at A (Theorem II, moment of the M/EIM/EI area about that support):

t=(540.00)(12.000)+(2340.00)(7.750)+(810.00)(3.000)=27045.00EIt = (540.00)(12.000) + (2340.00)(7.750) + (810.00)(3.000) = \frac{27045.00}{EI}

That support does not deflect, so θA=−t/14\theta_A = -t/14:

θA=−1931.786EI (clockwise)\theta_A = \frac{-1931.786}{EI}\ \text{(clockwise)}

At the 120 kN load (x=3x = 3 m):

θ=θA+∑A=−1931.786+[(540.00)]=−1391.786EI (clockwise)\theta = \theta_A + \sum A = -1931.786 + [(540.00)] = \frac{-1391.786}{EI}\ \text{(clockwise)} y=θA x+tP/A=−5795.357+[(540.00)(1.000)]=−5255.357EI (downward)y = \theta_A\,x + t_{P/A} = -5795.357 + [(540.00)(1.000)] = \frac{-5255.357}{EI}\ \text{(downward)}

At the 80 kN load (x=9.5x = 9.5 m):

θ=θA+∑A=−1931.786+[(540.00)+(2340.00)]=948.214EI (anticlockwise)\theta = \theta_A + \sum A = -1931.786 + [(540.00) + (2340.00)] = \frac{948.214}{EI}\ \text{(anticlockwise)} y=θA x+tP/A=−18351.964+[(540.00)(7.500)+(2340.00)(3.250)]=−6696.964EI (downward)y = \theta_A\,x + t_{P/A} = -18351.964 + [(540.00)(7.500) + (2340.00)(3.250)] = \frac{-6696.964}{EI}\ \text{(downward)}

At the point of maximum deflection (x=6.866x = 6.866 m):

θ=θA+∑A=−1931.786+[(540.00)+(1391.76)]≈0 (horizontal tangent)\theta = \theta_A + \sum A = -1931.786 + [(540.00) + (1391.76)] \approx 0\ \text{(horizontal tangent)} y=θA x+tP/A=−13263.641+[(540.00)(4.866)+(1391.76)(1.933)]=−7945.729EI (downward)y = \theta_A\,x + t_{P/A} = -13263.641 + [(540.00)(4.866) + (1391.76)(1.933)] = \frac{-7945.729}{EI}\ \text{(downward)}

Maximum deflection

Between the loads the bending moment is constant, M=360M = 360 kNm, so the slope changes by 360/EI360/EI per metre. The slope is −1391.79/EI-1391.79/EI under the 120 kN load (x=3x = 3 m), so it is zero at

−1391.79+360 (x−3)=0  ⇒  x=6.866 m from A-1391.79 + 360\,(x - 3) = 0 \;\Rightarrow\; x = 6.866\ \text{m from A}

where the deflection is ymax=7945.7EIy_{max} = \dfrac{7945.7}{EI} downward (same formula as above).

Numerical values with EI=3.36×105EI = 3.36\times10^5 kNm2^2

PointSlope (rad)Deflection (mm)
A0.00575 (clockwise)0
Under 120 kN0.00414 (clockwise)15.64 down
Under 80 kN0.00282 (anticlockwise)19.93 down
B0.00523 (anticlockwise)0
Maximum, at 6.866 m from A023.65 down

Part 2: Verification by the conjugate beam method

Step 1: Reactions

RA=120.00R_{A} = 120.00 kN, RB=80.00R_{B} = 80.00 kN (positive = upward; check: ∑Fy=200.00\sum F_y = 200.00 kN equals the total load 200.00 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 3120x120 xEI540.002.000
3 to 9.5360360EI2340.006.250
9.5 to 141120−80x1120 - 80 xEI810.0011.000

(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 conjugate of a simply supported beam is a simply supported beam of the same span. 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=14x = 14 m (conjugate moment is zero there):

RA′×14=(540.00)(12.000)+(2340.00)(7.750)+(810.00)(3.000)=27045.00R'_A\times14 = (540.00)(12.000) + (2340.00)(7.750) + (810.00)(3.000) = 27045.00 RA′=1931.786EI (slope at A, clockwise)R'_A = \frac{1931.786}{EI}\ \text{(slope at A, clockwise)}

At the 120 kN load (x=3x = 3 m):

V′=RA′−∑A=1931.786−[(540.00)]=1391.786EI (slope, clockwise)V' = R'_A - \sum A = 1931.786 - [(540.00)] = \frac{1391.786}{EI}\ \text{(slope, clockwise)} M′=RA′ x−∑A(x−xˉ)=5795.357−[(540.00)(1.000)]=5255.357EI (deflection, downward)M' = R'_A\,x - \sum A(x-\bar x) = 5795.357 - [(540.00)(1.000)] = \frac{5255.357}{EI}\ \text{(deflection, downward)}

At the 80 kN load (x=9.5x = 9.5 m):

V′=RA′−∑A=1931.786−[(540.00)+(2340.00)]=−948.214EI (slope, anticlockwise)V' = R'_A - \sum A = 1931.786 - [(540.00) + (2340.00)] = \frac{-948.214}{EI}\ \text{(slope, anticlockwise)} M′=RA′ x−∑A(x−xˉ)=18351.964−[(540.00)(7.500)+(2340.00)(3.250)]=6696.964EI (deflection, downward)M' = R'_A\,x - \sum A(x-\bar x) = 18351.964 - [(540.00)(7.500) + (2340.00)(3.250)] = \frac{6696.964}{EI}\ \text{(deflection, downward)}

The conjugate beam gives the same slopes and deflections as the moment-area method, so the results are verified.

Answer: slope at A =0.00575= 0.00575 rad (clockwise); under the 120 kN load: slope 0.004140.00414 rad (clockwise), deflection 15.6415.64 mm downward; under the 80 kN load: slope 0.002820.00282 rad (anticlockwise), deflection 19.9319.93 mm downward. Maximum deflection =23.65= 23.65 mm downward at 6.8666.866 m from the left support.

✓ Answer checked by Claude Opus 5.5 (high effort)

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