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In-Place Hot-Mix Asphalt Density Estimation Using Ground-Penetrating Radar

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This research proposes the innovative use of ground-penetrating radar (GPR) for effectively, continuously, and rapidly estimating in-place hotmix asphalt (HMA) density. On the basis of electromagnetic mixing theories, three candidate models were developed to determine HMA's dielectric constant, considering dielectric and volumetric properties of its three major components of HMA: air, binder, and aggregate. Laboratory tests were conducted on midsize HMA slabs (60 cm × 60 cm × 7.5 cm) to evaluate the models. After evaluating and comparing the three models, it was determined that the prediction model based on the Rayleigh mixing theory was the most accurate. The selected model was calibrated with a field core and then validated using field GPR measurements of a composite pavement with an HMA surface. The selected model provided accurate HMA density within a reasonable range.
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... The main issue in this method is estimation of the velocity ν of electromagnetic (EM) wave in the layers [2]. The wave velocity in each layer is proportional to the square root of the permittivity ϵ of that layer [9], [15]. In monostatic configuration, the thickness h of a layer can be calculated by h = ν∆τ/2 where ∆τ is the time difference between the received echoes. ...
... We simulate the reflection coefficient of the antenna placed above an asphalt layer with relative permittivity of ϵ ′ 1 = [2, 6,9], conductivity of σ 1 = 0.04 S/m and thickness of h 1 = [1,4,7] cm. Thickness of the asphalt sub-layer is considered to be infinite and its relative permittivity is set equal to 4. We used the result of these simulations as the measurement data in the cost function defined by (33). ...
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p>A fast analytical model for prediction of antenna S<sub>11</sub> in presence of a layered medium; This model is based on plane wave expansion of antenna field and has two appriximations. The first is neglecting the evanescent modes of plane wave and the second is neglecting the multiple reflections from the antenna to the multilayer.</p
... The main issue in this method is estimation of the velocity ν of electromagnetic (EM) wave in the layers [2]. The wave velocity in each layer is proportional to the square root of the permittivity ϵ of that layer [9], [15]. In monostatic configuration, the thickness h of a layer can be calculated by h = ν∆τ/2 where ∆τ is the time difference between the received echoes. ...
... We simulate the reflection coefficient of the antenna placed above an asphalt layer with relative permittivity of ϵ ′ 1 = [2, 6,9], conductivity of σ 1 = 0.04 S/m and thickness of h 1 = [1,4,7] cm. Thickness of the asphalt sub-layer is considered to be infinite and its relative permittivity is set equal to 4. We used the result of these simulations as the measurement data in the cost function defined by (33). ...
Preprint
Full-text available
p>A fast analytical model for prediction of antenna S<sub>11</sub> in presence of a layered medium; This model is based on plane wave expansion of antenna field and has two appriximations. The first is neglecting the evanescent modes of plane wave and the second is neglecting the multiple reflections from the antenna to the multilayer.</p
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