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Structural Beam Bending & Stress Inversion (Mechanical Engineering) Solution

1. Zero-Moment Pinning Stations (xx-Intercepts)

  1. Name the Governing Formula: The Factorization of Polynomial Roots:
    M(x)=0M(x) = 0
  2. Solve for xx on [0,6][0, 6]: Factor out the common term 2x2x:
    2x3βˆ’18x2+40x=0β€…β€ŠβŸΉβ€…β€Š2x(x2βˆ’9x+20)=02x^3 - 18x^2 + 40x = 0 \implies 2x(x^2 - 9x + 20) = 0
    Factor the quadratic term:
    2x(xβˆ’4)(xβˆ’5)=02x(x - 4)(x - 5) = 0
    The roots within the girder span are:
    x=0Β m,x=4Β m,x=5Β mx = 0\text{ m}, \quad x = 4\text{ m}, \quad x = 5\text{ m}
    The bending moment passes through zero at the girder left support (x=0x = 0), and at intermediate load crossover stations at x=4Β mx = 4\text{ m} and x=5Β mx = 5\text{ m}.

2. Shear Force & Extreme Bending Moments

  1. Name the Governing Formula: The Beam Differential Equilibrium Relation (V(x)=Mβ€²(x)V(x) = M'(x)) and the First Derivative Test for Local Extrema: (Defined in First Derivative Test.)
  2. Differentiate M(x)M(x):
    Mβ€²(x)=ddx[2x3βˆ’18x2+40x]=6x2βˆ’36x+40M'(x) = \frac{d}{dx}[2x^3 - 18x^2 + 40x] = 6x^2 - 36x + 40
  3. Locate Critical Numbers: Set Mβ€²(x)=0M'(x) = 0:
    6x2βˆ’36x+40=0β€…β€ŠβŸΉβ€…β€Š3x2βˆ’18x+20=06x^2 - 36x + 40 = 0 \implies 3x^2 - 18x + 20 = 0
    Apply the Quadratic Formula:
    x=βˆ’(βˆ’18)Β±(βˆ’18)2βˆ’4(3)(20)2(3)=18Β±324βˆ’2406=18Β±846=3Β±2216=3Β±213x = \frac{-(-18) \pm \sqrt{(-18)^2 - 4(3)(20)}}{2(3)} = \frac{18 \pm \sqrt{324 - 240}}{6} = \frac{18 \pm \sqrt{84}}{6} = 3 \pm \frac{2\sqrt{21}}{6} = 3 \pm \frac{\sqrt{21}}{3}
    Numerical values (21β‰ˆ4.5826\sqrt{21} \approx 4.5826):
    x1=3βˆ’1.5275β‰ˆ1.472Β m,x2=3+1.5275β‰ˆ4.528Β mx_1 = 3 - 1.5275 \approx 1.472\text{ m}, \qquad x_2 = 3 + 1.5275 \approx 4.528\text{ m}
    Both critical points lie within the girder span [0,6][0, 6].
  4. Sign Chart and Classification: Because Mβ€²(x)=6x2βˆ’36x+40M'(x) = 6x^2 - 36x + 40 is a parabola opening upward:
    • For x∈[0,1.472)x \in [0, 1.472): Mβ€²(x)>0β€…β€ŠβŸΉβ€…β€ŠMM'(x) > 0 \implies M is increasing.
    • For x∈(1.472,4.528)x \in (1.472, 4.528): Mβ€²(x)<0β€…β€ŠβŸΉβ€…β€ŠMM'(x) < 0 \implies M is decreasing.
    • For x∈(4.528,6]x \in (4.528, 6]: Mβ€²(x)>0β€…β€ŠβŸΉβ€…β€ŠMM'(x) > 0 \implies M is increasing.
    • At x1β‰ˆ1.472Β mx_1 \approx 1.472\text{ m}: Mβ€²M' changes +β†’βˆ’β€…β€ŠβŸΉβ€…β€Š+ \to -\implies Local Maximum Bending Moment:
      M(1.472)β‰ˆ2(1.472)3βˆ’18(1.472)2+40(1.472)β‰ˆ6.376βˆ’39.006+58.880β‰ˆ+26.25Β kNβ‹…mM(1.472) \approx 2(1.472)^3 - 18(1.472)^2 + 40(1.472) \approx 6.376 - 39.006 + 58.880 \approx +26.25\text{ kN}\cdot\text{m}
    • At x2β‰ˆ4.528Β mx_2 \approx 4.528\text{ m}: Mβ€²M' changes βˆ’β†’+β€…β€ŠβŸΉβ€…β€Š- \to +\implies Local Minimum Bending Moment:
      M(4.528)β‰ˆ2(4.528)3βˆ’18(4.528)2+40(4.528)β‰ˆ185.70βˆ’369.04+181.12β‰ˆβˆ’2.22Β kNβ‹…mM(4.528) \approx 2(4.528)^3 - 18(4.528)^2 + 40(4.528) \approx 185.70 - 369.04 + 181.12 \approx -2.22\text{ kN}\cdot\text{m}

3. Second Derivative & Inflection Points

  1. Name the Governing Formula: The Second Derivative Inflection Criterion:
    Mβ€²β€²(x)=0withΒ concavityΒ signΒ transitionM''(x) = 0 \quad \text{with concavity sign transition}
    (Defined in Concavity and the Second Derivative Test.)
  2. Compute Mβ€²β€²(x)M''(x):
    Mβ€²β€²(x)=ddx[6x2βˆ’36x+40]=12xβˆ’36=12(xβˆ’3)M''(x) = \frac{d}{dx}[6x^2 - 36x + 40] = 12x - 36 = 12(x - 3)
  3. Solve Mβ€²β€²(x)=0M''(x) = 0:
    12(xβˆ’3)=0β€…β€ŠβŸΉβ€…β€Šx=3Β m12(x - 3) = 0 \implies x = 3\text{ m}
  4. Concavity Sign Chart on [0,6][0, 6]:
    • On [0,3)[0, 3): Mβ€²β€²(x)<0β€…β€ŠβŸΉβ€…β€ŠM''(x) < 0 \implies Concave Downward (∩\cap).
    • On (3,6](3, 6]: Mβ€²β€²(x)>0β€…β€ŠβŸΉβ€…β€ŠM''(x) > 0 \implies Concave Upward (βˆͺ\cup).
  5. Inflection Point Coordinates: Because Mβ€²β€²(x)M''(x) transitions strictly from negative to positive across x=3x = 3:
    M(3)=2(3)3βˆ’18(3)2+40(3)=54βˆ’162+120=+12Β kNβ‹…mM(3) = 2(3)^3 - 18(3)^2 + 40(3) = 54 - 162 + 120 = +12\text{ kN}\cdot\text{m}
    The inflection point is located at (3,12)(3, 12).

4. Structural Engineering Significance

In structural mechanics, the derivative of bending moment is shear force (V(x)=Mβ€²(x)V(x) = M'(x)), and the second derivative is the distributed load intensity (w(x)=βˆ’Mβ€²β€²(x)w(x) = -M''(x)). The inflection point at x=3Β mx = 3\text{ m} indicates where the rate of change of shear force passes through zero (dVdx=0\frac{dV}{dx} = 0), identifying the location of steepest shear gradient reversal along the girder web. Placing transverse web stiffeners near this inflection boundary prevents localized diagonal web buckling under heavy rolling crane loads.