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At least 649 records · Page 36

Multiphysics and Multiscale Modeling of Coupled Transport of Chloride Ions in Concrete

Chloride ions (Cl−)-induced corrosion is one of the main degradation mechanisms in reinforced concrete (RC) structures. In most situations, the degradation initiates with the transport of Cl− from the surface of the concrete towards the reinforcing steel. The accumulation of Cl− at the steel-concrete interface could initiate reinforcement corrosion once a threshold Cl− concentration is achieved. An accurate numerical model of the Cl− transport in concrete is required to predict the corrosion initiation in RC structures. However, existing numerical models lack a representation of the heterogenous concrete microstructure resulting from the varying environmental conditions and the indirect effect of time dependent temperature and relative humidity (RH) on the water adsorption and Cl− binding isotherms. In this study, a numerical model is developed to study the coupled transport of Cl− with heat, RH and oxygen (O2) into the concrete. The modeling of the concrete microstructure is performed using the Virtual Cement and Concrete Testing Laboratory (VCCTL) code developed by the U.S. National Institute of Standards and Technology (NIST). The concept of equivalent maturation time is utilized to eliminate the limitation of simulating concrete microstructure using VCCTL in specific environmental conditions such as adiabatic. Thus, a time-dependent concrete microstructure, which depends on the hydration reactions coupled with the temperature and RH of the environment, is achieved to study the Cl− transport. Additionally, Cl− binding isotherms, which are a function of the pH of the concrete pore solution, Cl− concentration, and weight fraction of mono-sulfate aluminate (AFm) and calcium-silicate-hydrate (C-S-H), obtained from an experimental study by the same authors are utilized to account for the Cl− binding of cement hydration products. The temperature dependent RH diffusion was considered to account for the transport of Cl− with moisture transport. The temperature and RH diffusion in the concrete domain, composite theory, and Cl− binding and water adsorption isotherms are used in combination, to estimate the ensuing Cl− diffusion field within the concrete. The coupled transport process of heat, RH, Cl−, and O2 is implemented in the Multiphysics Object-Oriented Simulation Environment (MOOSE) developed by the U.S. Idaho National Laboratory (INL). The model was verified and validated using data from multiple experimental studies with different concrete mixture proportions, curing durations, and environmental conditions. Additionally, a sensitivity analysis was performed to identify that the water-to-cement (w/c) ratio, the exposure duration, the boundary conditions: temperature, RH, surface Cl− concentration, Cl− diffusion coefficient in the capillary water, and the critical RH are the important parameters that govern the Cl− transport in RC structures. In a case study, the capabilities of the developed numerical model are demonstrated by studying the complex 2D diffusion of Cl− in a RC beam located in two different climatic regions: warm and humid weather in Galveston, Texas, and cold and dry weather in North Minnesota, Minnesota, subjected to time varying temperature, RH, and surface Cl− concentrations.

composite theory↗

Cloud Detection Using Measured and Modeled State Parameters

In this study, hourly RUC analyses were used to examine the differences between RH and temperature values from RUC reanalysis data and from radiosonde atmospheric profiles obtained at the ARM SCF. The results show that the temperature observations from the SONDE and RUC are highly correlated. The RHs are also well-correlated, but the SONDE values generally exceed those from RUC. Inside cloud layers, the RH from RUC is 2-14% lower than the RH from SONDE for all RUC layers. Although the layer mean RH within clouds is much greater than the layer mean RH outside cloud or in the clear-sky, RH thresholds chosen as a function of temperature can more accurately diagnose cloud occurrence for either dataset. For overcast clouds, it was found that the 50% probability RH threshold for diagnosing a cloud, within a given upper tropospheric layer is roughly 90% for the Vaisala RS80-15LH radisonde and 80% for RUC data. While for the partial cloud (cloud amount is less than 90%), the RH thresholds of SONDE are close to RUC for a given probability in upper tropospheric layers. The probabilities of detecting clouds at a given RH and temperature should be useful for a variety of application such as the development of new cloud parameterizations or for estimating the vertical profile of cloudiness underneath a given cloud observed from the satellite to construct a 3-D cloud data set for computing atmospheric radiative heating profiles or determining potential aircraft icing conditions.

Yi, Y.↗

Materials Data on Y2GeRh3 by Materials Project

Y2Rh3Ge crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Y is bonded in a 9-coordinate geometry to four equivalent Y, nine equivalent Rh, and three equivalent Ge atoms. There are one shorter (3.09 Å) and three longer (3.37 Å) Y–Y bond lengths. There are three shorter (2.93 Å) and six longer (3.21 Å) Y–Rh bond lengths. All Y–Ge bond lengths are 3.27 Å. Rh is bonded to six equivalent Y, four equivalent Rh, and two equivalent Ge atoms to form distorted RhY6Ge2Rh4 cuboctahedra that share corners with four equivalent GeY6Rh6 cuboctahedra, corners with fourteen equivalent RhY6Ge2Rh4 cuboctahedra, edges with six equivalent RhY6Ge2Rh4 cuboctahedra, faces with six equivalent GeY6Rh6 cuboctahedra, and faces with twelve equivalent RhY6Ge2Rh4 cuboctahedra. All Rh–Rh bond lengths are 2.81 Å. Both Rh–Ge bond lengths are 2.57 Å. Ge is bonded to six equivalent Y and six equivalent Rh atoms to form distorted GeY6Rh6 cuboctahedra that share corners with six equivalent GeY6Rh6 cuboctahedra, corners with twelve equivalent RhY6Ge2Rh4 cuboctahedra, edges with six equivalent GeY6Rh6 cuboctahedra, and faces with eighteen equivalent RhY6Ge2Rh4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on Ho2Ge2Rh by Materials Project

Ho2RhGe2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ho sites. In the first Ho site, Ho is bonded in a 8-coordinate geometry to two equivalent Rh and six Ge atoms. Both Ho–Rh bond lengths are 3.05 Å. There are a spread of Ho–Ge bond distances ranging from 2.99–3.09 Å. In the second Ho site, Ho is bonded in a 11-coordinate geometry to four equivalent Rh and seven Ge atoms. There are a spread of Ho–Rh bond distances ranging from 3.01–3.25 Å. There are a spread of Ho–Ge bond distances ranging from 2.98–3.30 Å. Rh is bonded in a 10-coordinate geometry to six Ho and four Ge atoms. There are a spread of Rh–Ge bond distances ranging from 2.50–2.72 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to seven Ho, one Rh, and one Ge atom. The Ge–Ge bond length is 2.63 Å. In the second Ge site, Ge is bonded in a 10-coordinate geometry to six Ho, three equivalent Rh, and one Ge atom. The Ge–Ge bond length is 2.69 Å.

36 MATERIALS SCIENCE↗

Materials Data on VAsRh by Materials Project

RhVAs crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. V is bonded in a 3-coordinate geometry to six equivalent Rh and five equivalent As atoms. There are a spread of V–Rh bond distances ranging from 2.90–2.96 Å. There are a spread of V–As bond distances ranging from 2.53–2.82 Å. Rh is bonded in a 12-coordinate geometry to six equivalent V, two equivalent Rh, and four equivalent As atoms. Both Rh–Rh bond lengths are 2.81 Å. There are a spread of Rh–As bond distances ranging from 2.40–2.52 Å. As is bonded in a 9-coordinate geometry to five equivalent V and four equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on SiRh2 by Materials Project

Rh2Si is Cotunnite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Rh sites. In the first Rh site, Rh is bonded to four equivalent Si atoms to form a mixture of distorted edge and corner-sharing RhSi4 tetrahedra. There are a spread of Rh–Si bond distances ranging from 2.42–2.47 Å. In the second Rh site, Rh is bonded in a 3-coordinate geometry to three equivalent Si atoms. There are one shorter (2.49 Å) and two longer (2.50 Å) Rh–Si bond lengths. Si is bonded in a 7-coordinate geometry to seven Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on La2InRh2 by Materials Project

La2Rh2In crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. La is bonded in a 6-coordinate geometry to six equivalent Rh and four equivalent In atoms. There are two shorter (2.92 Å) and four longer (3.10 Å) La–Rh bond lengths. All La–In bond lengths are 3.49 Å. Rh is bonded in a 2-coordinate geometry to six equivalent La, one Rh, and two equivalent In atoms. The Rh–Rh bond length is 2.91 Å. Both Rh–In bond lengths are 3.01 Å. In is bonded to eight equivalent La and four equivalent Rh atoms to form a mixture of corner and face-sharing InLa8Rh4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on SbRh2 by Materials Project

Rh2Sb is Cotunnite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 3-coordinate geometry to five equivalent Sb atoms. There are a spread of Rh–Sb bond distances ranging from 2.68–2.99 Å. In the second Rh site, Rh is bonded to five equivalent Sb atoms to form a mixture of distorted edge and corner-sharing RhSb5 tetrahedra. There are a spread of Rh–Sb bond distances ranging from 2.61–3.27 Å. Sb is bonded in a 10-coordinate geometry to ten Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on BRh2 by Materials Project

Rh2B is Cotunnite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a distorted trigonal non-coplanar geometry to three equivalent B atoms. There are one shorter (2.09 Å) and two longer (2.34 Å) Rh–B bond lengths. In the second Rh site, Rh is bonded in a 4-coordinate geometry to four equivalent B atoms. There are a spread of Rh–B bond distances ranging from 2.12–2.47 Å. B is bonded in a 7-coordinate geometry to seven Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ce3(GeRh)2 by Materials Project

Ce3Rh2Ge2 crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 9-coordinate geometry to four equivalent Rh and five Ge atoms. There are two shorter (3.08 Å) and two longer (3.10 Å) Ce–Rh bond lengths. There are a spread of Ce–Ge bond distances ranging from 3.03–3.34 Å. In the second Ce site, Ce is bonded in a 8-coordinate geometry to four equivalent Rh and five Ge atoms. There are a spread of Ce–Rh bond distances ranging from 2.86–3.22 Å. There are a spread of Ce–Ge bond distances ranging from 3.10–3.40 Å. Rh is bonded in a 9-coordinate geometry to six Ce and three Ge atoms. There are a spread of Rh–Ge bond distances ranging from 2.56–2.68 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 12-coordinate geometry to eight Ce and four equivalent Rh atoms. In the second Ge site, Ge is bonded in a 9-coordinate geometry to seven Ce and two equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on GeRh2 by Materials Project

Rh2Ge is Cotunnite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Rh sites. In the first Rh site, Rh is bonded to five equivalent Ge atoms to form a mixture of distorted edge and corner-sharing RhGe5 tetrahedra. There are a spread of Rh–Ge bond distances ranging from 2.50–3.06 Å. In the second Rh site, Rh is bonded in a 3-coordinate geometry to five equivalent Ge atoms. There are a spread of Rh–Ge bond distances ranging from 2.55–2.88 Å. Ge is bonded in a 10-coordinate geometry to ten Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on P2Rh3 by Materials Project

Rh3P2 crystallizes in the tetragonal P-4m2 space group. The structure is three-dimensional. there are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 4-coordinate geometry to four equivalent P atoms. All Rh–P bond lengths are 2.33 Å. In the second Rh site, Rh is bonded in a 5-coordinate geometry to five equivalent P atoms. There are one shorter (2.36 Å) and four longer (2.48 Å) Rh–P bond lengths. P is bonded to seven Rh atoms to form a mixture of distorted edge, corner, and face-sharing PRh7 pentagonal bipyramids.

36 MATERIALS SCIENCE↗

Materials Data on Y2Si2Rh by Materials Project

Y2RhSi2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 2-coordinate geometry to four equivalent Rh and six Si atoms. There are a spread of Y–Rh bond distances ranging from 3.06–3.15 Å. There are a spread of Y–Si bond distances ranging from 2.92–3.07 Å. In the second Y site, Y is bonded in a 6-coordinate geometry to two equivalent Rh and six Si atoms. Both Y–Rh bond lengths are 3.26 Å. There are a spread of Y–Si bond distances ranging from 2.90–3.16 Å. Rh is bonded in a 4-coordinate geometry to six Y and four Si atoms. There are a spread of Rh–Si bond distances ranging from 2.45–2.59 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to five Y, three equivalent Rh, and one Si atom. The Si–Si bond length is 2.62 Å. In the second Si site, Si is bonded in a 9-coordinate geometry to seven Y, one Rh, and one Si atom. The Si–Si bond length is 2.56 Å.

36 MATERIALS SCIENCE↗

Materials Data on Sm2GeRh3 by Materials Project

Sm2Rh3Ge crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Sm is bonded in a 9-coordinate geometry to four equivalent Sm, nine equivalent Rh, and three equivalent Ge atoms. There are one shorter (3.10 Å) and three longer (3.40 Å) Sm–Sm bond lengths. There are three shorter (2.96 Å) and six longer (3.23 Å) Sm–Rh bond lengths. All Sm–Ge bond lengths are 3.31 Å. Rh is bonded to six equivalent Sm, four equivalent Rh, and two equivalent Ge atoms to form distorted RhSm6Ge2Rh4 cuboctahedra that share corners with four equivalent GeSm6Rh6 cuboctahedra, corners with fourteen equivalent RhSm6Ge2Rh4 cuboctahedra, edges with six equivalent RhSm6Ge2Rh4 cuboctahedra, faces with six equivalent GeSm6Rh6 cuboctahedra, and faces with twelve equivalent RhSm6Ge2Rh4 cuboctahedra. All Rh–Rh bond lengths are 2.84 Å. Both Rh–Ge bond lengths are 2.59 Å. Ge is bonded to six equivalent Sm and six equivalent Rh atoms to form distorted GeSm6Rh6 cuboctahedra that share corners with six equivalent GeSm6Rh6 cuboctahedra, corners with twelve equivalent RhSm6Ge2Rh4 cuboctahedra, edges with six equivalent GeSm6Rh6 cuboctahedra, and faces with eighteen equivalent RhSm6Ge2Rh4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on Y3(SiRh)2 by Materials Project

Y3(RhSi)2 crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 6-coordinate geometry to four equivalent Rh and five Si atoms. There are a spread of Y–Rh bond distances ranging from 2.90–3.10 Å. There are a spread of Y–Si bond distances ranging from 2.96–3.40 Å. In the second Y site, Y is bonded in a 9-coordinate geometry to four equivalent Rh and five Si atoms. There are two shorter (3.02 Å) and two longer (3.10 Å) Y–Rh bond lengths. There are a spread of Y–Si bond distances ranging from 2.97–3.28 Å. Rh is bonded in a 9-coordinate geometry to six Y and three Si atoms. There are a spread of Rh–Si bond distances ranging from 2.49–2.52 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to seven Y and two equivalent Rh atoms. In the second Si site, Si is bonded in a 12-coordinate geometry to eight Y and four equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on TiAsRh by Materials Project

TiRhAs crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ti is bonded in a 11-coordinate geometry to six equivalent Rh and five equivalent As atoms. There are a spread of Ti–Rh bond distances ranging from 2.93–3.08 Å. There are a spread of Ti–As bond distances ranging from 2.66–2.80 Å. Rh is bonded in a 12-coordinate geometry to six equivalent Ti, two equivalent Rh, and four equivalent As atoms. Both Rh–Rh bond lengths are 2.83 Å. There are a spread of Rh–As bond distances ranging from 2.44–2.56 Å. As is bonded in a 9-coordinate geometry to five equivalent Ti and four equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on Bi9Rh2I3 by Materials Project

Rh2Bi9I(I)2 crystallizes in the monoclinic P2_1/m space group. The structure is one-dimensional and consists of four hydriodic acid molecules and one Rh2Bi9I ribbon oriented in the (0, 1, 0) direction. In the Rh2Bi9I ribbon, Rh is bonded in a 8-coordinate geometry to eight Bi atoms. There are a spread of Rh–Bi bond distances ranging from 2.80–2.92 Å. There are six inequivalent Bi sites. In the first Bi site, Bi is bonded in a distorted L-shaped geometry to two equivalent Rh atoms. In the second Bi site, Bi is bonded in an L-shaped geometry to two equivalent Rh and one Bi atom. The Bi–Bi bond length is 3.27 Å. In the third Bi site, Bi is bonded in a 2-coordinate geometry to two equivalent Rh, three Bi, and one I atom. Both Bi–Bi bond lengths are 3.24 Å. The Bi–I bond length is 3.54 Å. In the fourth Bi site, Bi is bonded in a distorted single-bond geometry to one Rh and one Bi atom. In the fifth Bi site, Bi is bonded in a 6-coordinate geometry to two equivalent Rh atoms. In the sixth Bi site, Bi is bonded in a 7-coordinate geometry to two equivalent Rh atoms. I is bonded in a distorted single-bond geometry to one Bi atom.

36 MATERIALS SCIENCE↗

Materials Data on Bi3Rh by Materials Project

RhBi3 crystallizes in the orthorhombic Pnma space group. The structure is one-dimensional and consists of two RhBi3 ribbons oriented in the (1, 0, 0) direction. Rh is bonded in a 9-coordinate geometry to two equivalent Rh and seven Bi atoms. Both Rh–Rh bond lengths are 2.87 Å. There are a spread of Rh–Bi bond distances ranging from 2.79–2.89 Å. There are three inequivalent Bi sites. In the first Bi site, Bi is bonded in a single-bond geometry to one Rh atom. In the second Bi site, Bi is bonded in a 3-coordinate geometry to three equivalent Rh atoms. In the third Bi site, Bi is bonded in a 3-coordinate geometry to three equivalent Rh atoms.

36 MATERIALS SCIENCE↗