Bridge
Vehicle
Road roughness
Live animation
Mid-span deflection
Vehicle vertical acceleration
Frequency content
Method
The bridge is modeled as a simply supported Euler-Bernoulli beam with mode shapes φn(x) = sin(nπx/L) and natural frequencies ωn = (nπ/L)² √(EI/m̄). The beam response is expanded as w(x,t) = Σ qn(t) φn(x).
The vehicle is a quarter-car: a sprung mass ms coupled to an unsprung mass mu by a parallel spring-damper (ks, cs), with the unsprung mass connected to the contact point through tire spring-damper (kt, ct). The contact-point elevation is w(p(t), t) + r(p(t)), with p(t) = vt and r a ISO 8608 random roughness profile generated from a discrete inverse-FFT of the displacement PSD Gd(n) = Gd(n0) · (n/n0)-2.
The coupled equations include the convective term v · ∂w/∂x at the contact point. The full mass/damping/stiffness matrices are time-varying through φ(p(t)) and are integrated with the constant-average-acceleration Newmark-beta scheme (γ = 1/2, β = 1/4).
The FFT panel illustrates the indirect identification principle: peaks in the sprung-mass acceleration spectrum cluster around the bridge natural frequencies, which is the core observation underlying crowdsensing-based bridge monitoring.
Related publications
- Talebi-Kalaleh, M.; Gül, M.; Mei, Q. (2025). Crowdsensing-based Bridge Vibration Monitoring Using a Sparse Network of Random Mobile Sensors. Journal of Sound and Vibration, 618B. DOI
- Talebi-Kalaleh, M.; Mei, Q. (2026). An Open-Source Framework for Coupled Vehicle-Bridge Interaction Analysis Using OpenSees. arXiv:2605.09175. arXiv
- Talebi-Kalaleh, M.; Mei, Q. (2023). A Mobile Sensing Framework for Bridge Modal Identification. Sensors, 23(11), 5154. DOI