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Sandbox Physics

M023 · Structural mechanics

Truss Bridge Force Explorer

What is the least material a truss bridge needs to carry a load anywhere on its deck? Just enough that, with the load in its worst position, no member exceeds its tension strength or buckles in compression. Each member's worst position is different, so move the load across the whole deck instead of checking only the middle.

Build a Warren truss or a reinforced planar truss, move the load along it and measure the displacement. Compare tension, compression and buckling of the pin-ended members as the load crosses the whole deck.

Interactive modelTruss Bridge Force Explorer
Model domain—\text{—}
Left vertical reaction—\text{—}
Right vertical reaction—\text{—}
Largest displacement magnitude—\text{—}
Probe vertical displacement—\text{—}
Maximum axial stress magnitude—\text{—}
Largest ideal utilization—\text{—}
Elastic strain energy—\text{—}
Cross-section area—\text{—}
Section second moment—\text{—}
Actual displacement display gain—\text{—}
Acquired load stations—\text{—}
Modulus fitted from raw data—\text{—}
Fit residual RMS—\text{—}
Inspected member number—\text{—}
Selected axial force: tension positive—\text{—}
Selected unloaded length—\text{—}
Selected axial stress—\text{—}
Selected ideal pinned buckling load—\text{—}
Horizontal pin reaction—\text{—}
Free-node equilibrium residual—\text{—}
Minimum equal rod area—\text{—}
Minimum rod material volume—\text{—}
Verified deck-node load cases—\text{—}

Physics tutorial

Follow the load path, then measure its compliance

BackgroundThe load is applied slowly, so the truss stays in equilibrium and inertia can be ignored.

Why it mattersMIT notes on mechanics of materials derive joint equilibrium, axial elasticity and Euler–Bernoulli bending from the same force balance and energy argument.

Start with the essentials

Focus question
What is the least material that can carry the load at every position?
One-sentence intuition
The geometry decides which members carry the load; the cross-section and the modulus decide how far the truss gives under it.

Core mathematical model

Joint equilibrium

Kffuf=ff\mathbf K_{ff}\mathbf u_f=\mathbf f_f

Only the free joint motions are solved for. The left pin blocks motion in both directions; the right roller blocks only vertical motion.

Axial rod law

Ne=EAℓeΔℓe,σe=NeAN_e=\frac{EA}{\ell_e}\Delta\ell_e,\qquad\sigma_e=\frac{N_e}{A}

A rod stretches by the difference of its two end displacements, projected onto the unloaded rod direction. A positive force means tension.

Two separate limits: yield and buckling

∣Ne∣≤Aσys,−Ne≤π2EIsℓe2|N_e|\leq\frac{A\sigma_y}{s},\qquad -N_e\leq\frac{\pi^2EI}{s\ell_e^2}

The second condition applies only to rods in compression, treated as ideal straight rods with pinned ends. The design safety factor is 1.5.

Material volume of solid round rods

I=A24π,V=A∑eℓeI=\frac{A^2}{4\pi},\qquad\mathcal V=A\sum_e\ell_e

The smallest common rod area must meet the strength and displacement limits with the load at every deck joint. A load between two joints gives a convex combination of those two cases, so the joint cases cover it.

Independent energy check

U=∑eNe2ℓe2EA=12fTuU=\sum_e\frac{N_e^2\ell_e}{2EA}=\frac12\mathbf f^{\mathsf T}\mathbf u

When a linear elastic truss is loaded gradually, the axial strain energy in the rods must equal half the work of the external forces through their displacements.

Common difficulties

The drawn bend is magnified

Typical misconceptionHow far the bridge bends on screen is how far it really moves.

Better mental modelRead the displacement from the readouts or the plot. The 3D display gain only changes how the deformation is drawn.

Past a limit, the model does not show collapse

Typical misconceptionA rod or beam pushed past an ideal limit still behaves as this linear model says.

Better mental modelRead a red solution as an extrapolation. The model leaves out plastic flow and what happens after buckling.

The modulus comes from the data

Typical misconceptionThe fitted modulus just copies the reference slider.

Better mental modelDelete the recorded data and the estimate disappears. Record several loads and change the noise to see how well the modulus is recovered.

Run the experiment

  1. 01

    Change the load path

    Compare the Warren truss and Reinforced web presets.

    What to observe: The support reactions and the member forces change together.
  2. 02

    Move the load and probe

    Drag the two colored station handles below the bridge.

    What to observe: The probe reads the physical deflection. Moving it clears earlier measurements that no longer match the new position.
  3. 03

    Measure the material

    Use Acquire nine load steps, add bounded sensor noise, then Export raw observations.

    What to observe: The fitted slope gives the modulus, and the residuals show how much the sensor readings scatter.
  4. 04

    Find the minimum rod area

    Use Check all deck load stations, then Use minimum equal rod section.

    What to observe: The minimum-area search checks both strength and the deflection allowed in service.
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