Multi-Station Beam Reaction Test Bed
Rigid structural bed supporting simply supported beam across a 1000 mm span.
Verify the Maxwell–Betti reciprocal deflection theorem on an elastic simply supported beam by comparing deflection at station A due to load at station B (δ_AB) with deflection at station B due to load at station A (δ_BA). Explore interactive structural mechanics, materials simulation, and civil engineering telemetry.
Ready to sample with Applied Load = 15.0 kN.
Adjust Applied Load, then execute civil engineering measurement.
Civil engineering telemetry is evaluated rigorously using 64-bit IEEE 754 precision. Residuals reflect ordinary least-squares regression across successive observations. Continuous data structures support high-fidelity structural mechanics and geotechnical continuum modeling.
The civil engineering physical models apply within the specified calibrated operational window (5.0 to 25.0 kN). Beam span L = 1000 mm. Station A located at x_A = 300 mm; Station B located at x_B = 600 mm. Closed-form flexibility coefficient f_AB = x_A (L - x_B) (2 L x_B - x_A^2 - x_B^2) / (6 E I L) = 0.3150 mm/kN.
Rigid structural bed supporting simply supported beam across a 1000 mm span.
Independent displacement transducers mounted at station A (300 mm) and station B (600 mm).
Applies concentrated vertical loads up to 30 kN with precision electronic load cell.
Uniform, homogeneous prismatic steel beam with known flexural rigidity EI.
Clamps LVDTs rigidly to isolated datum beam to prevent frame deflection errors.
Marks exact load and displacement stations to within 0.1 mm precision.
Verify the Maxwell–Betti reciprocal deflection theorem on an elastic simply supported beam by comparing deflection at station A due to load at station B (δ_AB) with deflection at station B due to load at station A (δ_BA). Standardized parameter settings: 5.0, 10.0, 15.0, 20.0, 25.0 kN.
Set beam clear span L = 1000.0 mm; mark Station A at x_A = 300.0 mm and Station B at x_B = 600.0 mm; position digital LVDTs at stations A and B; zero both gauges.
Position loading jack at Station B (x_B = 600 mm); apply loads P_B incrementally at 5.0, 10.0, 15.0, 20.0, and 25.0 kN.
At each load step, record deflection at Station A (δ_AB) and direct deflection at Station B (δ_BB); release load completely.
Verify both transducers return to zero (residual deflection < 0.005 mm) confirming purely elastic response.
Move loading jack to Station A (x_A = 300 mm); apply identical loads P_A at 5.0, 10.0, 15.0, 20.0, and 25.0 kN.
Record deflection at Station B (δ_BA) and direct deflection at Station A (δ_AA); compare δ_AB with δ_BA at every load step to verify reciprocity.
Points are your recorded observations. The solid regression line validates Maxwell-Betti Reciprocity mathematical scaling.
| # | Reciprocal Test Load P (kN) | Cross-Station Deflection δ_AB (mm) | Applied load P_B at station B (kN) | Measured deflection δ_AB at station A (mm) | Remove |
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No readings yet. Execute a civil engineering trial and record it.
The Maxwell–Betti reciprocal work theorem forms one of the foundational cornerstones of linear structural analysis, energy methods, and modern matrix structural mechanics. Formulated by James Clerk Maxwell in 1864 and generalized by Enrico Betti in 1872, the theorem states: For any linear elastic structure subjected to two independent equilibrium load systems, the work done by the first system acting through the displacements produced by the second system is identically equal to the work done by the second system acting through the displacements produced by the first system. When applied to two discrete load points A and B on a structural beam, the theorem simplifies to the classical reciprocal deflection law: the deflection at station A caused by a unit load at station B (flexibility coefficient f_AB) is identically equal to the deflection at station B caused by a unit load at station A (f_BA), meaning the global structural flexibility matrix is perfectly symmetric: [F] = [F]^T. This mathematical symmetry drastically reduces computational effort in structural indeterminate frame analysis and validates Müller-Breslau influence line principles. In this laboratory experiment, twin digital displacement transducers monitor reciprocal deflections across asymmetric beam stations to verify Maxwell-Betti reciprocity across loads from 5 to 25 kN.
Beam span L = 1000 mm. Station A located at x_A = 300 mm; Station B located at x_B = 600 mm. Closed-form flexibility coefficient f_AB = x_A (L - x_B) (2 L x_B - x_A^2 - x_B^2) / (6 E I L) = 0.3150 mm/kN.