AASHTO T 342-2011 Standard Method of Test for Determining Dynamic Modulus of Hot Mix Asphalt (HMA).pdf
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1、Standard Method of Test for Determining Dynamic Modulus of Hot Mix Asphalt (HMA) AASHTO Designation: T 342-11 (2015)1American Association of State Highway and Transportation Officials 444 North Capitol Street N.W., Suite 249 Washington, D.C. 20001 TS-2d T 342-1 AASHTO Standard Method of Test for Det
2、ermining Dynamic Modulus of Hot Mix Asphalt (HMA) AASHTO Designation: T 342-11 (2015)11. SCOPE 1.1. This test method covers procedures for preparing and testing hot mix asphalt (HMA) to determine the dynamic modulus and phase angle over a range of temperatures and loading frequencies. 1.2. This stan
3、dard is applicable to laboratory-prepared specimens of mixtures with nominal maximum size aggregate less than or equal to 37.5 mm (1.48 in.). 1.3. This standard may involve hazardous material, operations, and equipment. This standard does not purport to address all of the safety concerns associated
4、with its use. It is the responsibility of the user of this procedure to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use. 2. REFERENCED DOCUMENTS 2.1. AASHTO Standards: R 30, Mixture Conditioning of Hot Mix Asphalt (HMA) T 166,
5、Bulk Specific Gravity (Gmb) of Compacted Hot Mix Asphalt (HMA) Using Saturated Surface-Dry Specimens T 209, Theoretical Maximum Specific Gravity (Gmm) and Density of Hot Mix Asphalt (HMA) T 269, Percent Air Voids in Compacted Dense and Open Asphalt Mixtures T 312, Preparing and Determining the Densi
6、ty of Asphalt Mixture Specimens by Means of the Superpave Gyratory Compactor 2.2. ASTM Standard: E4, Standard Practices for Force Verification of Testing Machines 2.3. Other Document: Chapra, Steven C. and Raymond P. Canale, Numerical Methods for Engineers, The McGraw-Hill Companies, Inc., New York,
7、 NY, 1985, pp. 404407. 3. TERMINOLOGY 3.1. Definitions: 3.1.1. complex modulus (E*)a complex number that defines the relationship between stress and strain for a linear viscoelastic material. 2015 by the American Association of State Highway and Transportation Officials.All rights reserved. Duplicat
8、ion is a violation of applicable law.TS-2d T 342-2 AASHTO 3.1.2. dynamic modulus (|E*|)the normal value of the complex modulus calculated by dividing the maximum (peak-to-peak) stress by the recoverable (peak-to-peak) axial strain for a material subjected to a sinusoidal loading. 3.1.3. phase angle
9、()the angle in degrees between a sinusoidal applied peak stress and the resulting peak strain in a controlled stress test. 4. SUMMARY OF METHOD 4.1. A sinusoidal (haversine) axial compressive stress is applied to a specimen of asphalt concrete at a given temperature and loading frequency. The applie
10、d stress and the resulting recoverable axial strain response of the specimen is measured and used to calculate the dynamic modulus and phase angle. 4.2. Figure 1 presents one schematic of the dynamic modulus test. Figure 1General Schematic of Dynamic Modulus Test Load CellAxialLVDTSpecimenHardenedSt
11、eel DisksGreased DoubleMembrane 2015 by the American Association of State Highway and Transportation Officials.All rights reserved. Duplication is a violation of applicable law.TS-2d T 342-3 AASHTO 5. SIGNIFICANCE AND USE 5.1. Dynamic modulus values measured over a range of temperatures and frequenc
12、ies of loading can be shifted into a master curve for characterizing asphalt concrete for pavement thickness design and performance analysis. 5.2. The values of dynamic modulus and phase angle can also be used as performance criteria for HMA design. 6. APPARATUS 6.1. Dynamic Modulus Test SystemA dyn
13、amic modulus test system consisting of a testing machine, environmental chamber, and measuring system. 6.2. Testing MachineA servohydraulic testing machine capable of producing a controlled haversine compressive loading. The testing machine should have a capability of applying load over a range of f
14、requencies from 0.1 to 25 Hz and stress level up to 2800 kPa (400 psi). For sinusoidal loads, the standard error of the applied load shall be less than 5 percent. The standard error of the applied load is a measure of the difference between the measured load data and the best-fit sinusoid. The stand
15、ard error of the load is defined in Equation 1. 21100%()4()niiioxxse Pnx=(1) where: se(P) = standard error of the applied load, xi= measured load at point i, ix = predicted load at point i from the best-fit sinusoid, n = total number of data points collected during test, and ox = amplitude of the be
16、st-fit sinusoid. 6.2.1. Environmental ChamberA chamber for controlling the test specimen at the desired temperature. The environmental chamber shall be capable of controlling the temperature of the specimen over a temperature range from 10 to 60C (14 to 140F) to an accuracy of 0.5C (1F). The chamber
17、 shall be large enough to accommodate the test specimen and a dummy specimen with thermocouple mounted at the center for temperature verification. 6.2.2. Measurement SystemThe system shall be fully computer-controlled, capable of measuring and recording the time history of the applied load and the a
18、xial deformations. The system shall be capable of measuring the period of the applied sinusoidal load and resulting deformations with a resolution of 0.5 percent. The accuracy and resolution of measurements are summarized in Table 1. Table 1Accuracy and Resolution of Measurement System Measurement R
19、ange Accuracy Resolution Load 0.12 to 25 kN Error 0.0 percent 0.0012 kN Deformation 1 mm Error 0.0025 mm 0.0002 mm Inherent phase lag between load and deformation Not specified 1 degree Not specified 2015 by the American Association of State Highway and Transportation Officials.All rights reserved.
20、Duplication is a violation of applicable law.TS-2d T 342-4 AASHTO 6.2.2.1. LoadThe load shall be measured with an electronic load cell in contact with one of the specimen caps. The load cell shall be calibrated in accordance with ASTM E4. The load measuring system shall have a minimum range of 0 to
21、25 kN (0 to 5600 lb) with a resolution of 1.2 N (0.24 lb). 6.2.2.2. Axial DeformationsAxial deformations shall be measured with linear variable differential transformers (LVDT) mounted between gauge points glued to the specimen, for example, as shown in Figure 2. The deformations shall be measured a
22、t two locations 180 degrees apart, three locations 120 degrees apart, or four locations 90 degrees apart. The measurement setup that calls for four locations set at 90 degrees apart has an advantage over the other two options in that, in case one LVDT does not function properly, LVDT and the LVDT on
23、 the opposite side can be dropped, and the remaining two LVDTs can be used to determine the average deformation. The LVDTs shall have a range of 0.5 mm (0.02 in.). The deformation measuring system shall have auto zero and selectable ranges as defined in Table 2. Table 2Deformation Measuring System R
24、equirements Range, mm (in.) Resolution, mm (in.) 0.5 (0.01969) 0.0100 (0.00039) 0.25 (0.00984) 0.0050 (0.00020) 0.125 (0.00492) 0.0025 (0.00010) 0.0625 (0.00246) 0.0010 (0.00004) Figure 2General Schematic of Gauge Points (not to scale) 6.2.3. Loading PlatensLoading platens, sized 104.5 0.5 mm, are r
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