2018
DOI: 10.1115/1.4041500
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Closed-Form Solution of Road Roughness-Induced Vehicle Energy Dissipation

Abstract: A major contributor to rolling resistance is road roughness-induced energy dissipation in vehicle suspension systems. We identify the parameters driving this dissipation via a combination of dimensional analysis and asymptotic analysis. We begin with a mechanistic model and basic random vibration theory to relate the statistics of road roughness profile and the dynamic properties of the vehicle to dissipated energy. Asymptotic analysis is then used to unravel the dependence of the dissipation on key vehicle an… Show more

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Cited by 14 publications
(10 citation statements)
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“…The starting point is the realization that the only source of dissipation is the damping mechanism within the Kelvin-Voigt suspension system. The expected value of the energy dissipation per travelled length, δ , considering the stochastic nature of the road profile, therefore reads (24) can be approximated using asymptotic analysis for a small unsprungto-sprung mass ratio [7], γ = m u /m s 1. This is achieved by first approximating the poles of H z (ω) for an undamped system as…”
Section: (A) Dissipated Energymentioning
confidence: 99%
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“…The starting point is the realization that the only source of dissipation is the damping mechanism within the Kelvin-Voigt suspension system. The expected value of the energy dissipation per travelled length, δ , considering the stochastic nature of the road profile, therefore reads (24) can be approximated using asymptotic analysis for a small unsprungto-sprung mass ratio [7], γ = m u /m s 1. This is achieved by first approximating the poles of H z (ω) for an undamped system as…”
Section: (A) Dissipated Energymentioning
confidence: 99%
“…The integral on the r.h.s. of equation (2.4) can be approximated using asymptotic analysis for a small unsprung-to-sprung mass ratio [7], γ = m u / m s ≪ 1. This is achieved by first approximating the poles of H z ( ω ) for an undamped system as ω 1 ≈ 1 − 1/2 β 2 γ and ω 2 ≈ β (1 + 1/2 β 2 γ ).…”
Section: Road Vehicle Interaction: a Spectral Stochastic Modelmentioning
confidence: 99%
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“…A Gaussian roughness profile, for instance, results in a normally distributed suspension motion with χ ¼ ffiffiffiffiffiffiffi ffi 2=π p (for other marginal probability distributions; see Louhghalam et al, 2015). A convenient asymptotic solution for Equation (43) has recently been proposed in the function of only the road roughness PSD parameters, gΩ w 0 À Á and w (Louhghalam et al, 2019):…”
Section: Unknownsmentioning
confidence: 99%
“…where H z S,i and H z U,i respectively denote the sprung mass and unsprung mass FRFs of the front i ¼ 1 ð Þand rear ði ¼ 2Þ suspension system, that is, from the solution of Equation (36). Since the integral expression in Equation (51) converges rapidly, an estimate of the energy dissipated in the suspension system can be obtained from an asymptotic solution of Equation 50for the quarter-car model (Louhghalam et al, 2019). Using the model invariants (30) and (32), this asymptotic model holds-in first order-for the front and rear suspension system as:…”
Section: Energy Dissipationmentioning
confidence: 99%