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Specific Gravity-Soil Mechanics and Foundations-Lecture 04 Slides-Civil and Environmental Engineering, Slides of Soil Mechanics and Foundations

This lecture is delivered by Dr. Lanbu Liu in University of Connecticut for course Soil Mechanics and Foundations. Specific Gravity, Phases of Soils, Soil Model, Three Phase Diagram, Weight-volume Relationships, Fully Saturated Soils, Dry Soils, Dr. Lanbo Liu, University of Connecticut, Soil Mechanics and Foundations

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2011/2012

Uploaded on 02/29/2012

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Download Specific Gravity-Soil Mechanics and Foundations-Lecture 04 Slides-Civil and Environmental Engineering and more Slides Soil Mechanics and Foundations in PDF only on Docsity! CE 240 Soil Mechanics & Foundations Lecture 2.2 Weight-Volume Relationships (Das, Ch. 3) Outline of this Lecture 1.Density, Unit weight, and Specific gravity (Gs) 2.Phases in soil (a porous medium) 3.Three phase diagram 4.Weight-volume relationships Specific Gravity (Gs) Specific gravity is defined as the ratio of unit weight (or density) of a given material to the unit weight (or density) of water since s w w w gG g γ ρ ρ γ ρ ρ = = = Specific Gravity • Expected Value for Gs Type of Soil Gs Sand 2.65 - 2.67 Silty sand 2.67 – 2.70 Inorganic clay 2.70 – 2.80 Soils with mica or iron 2.75 – 3.00 Organic soils < 2.00 Three Phases of Soils Naturally occurred soils always consist of solid particles, water, and air, so that soil has three phases: solid, liquid and gas. Fully Saturated Soils (Two phase) Water Solid Mineral Skeleton Fully Saturated Dry Soils (Two phase) [Oven Dried] Air Solid Dry SoilMineral Skeleton Three Phase Diagram Solid Air Water WT Ws Ww Wa~0 Vs Va Vw Vv VT Weight Volume Void ratio: e = Vv/Vs; Porosity n = Vv/Vt / 1 / 1 / 1 / 1 v v v t s t v v t v v v s t s v v s V V V V ne V V V V V n V V V V en V V V V V e = = = = − − − = = = = + + + Apparently, for the same material we always have e > n. For example, when the porosity is 0.5 (50%), the void ratio is 1.0 already. Solid Air Water WT Ws Ww Wa~0 Vs Va Vw Vv VT Degree of saturation: S =Vw/Vv x 100% Saturation is measured by the ratio of volume. Moisture content (Water content): w = Ww/Ws, Ww – weight of water, Ws – weight of solid Water content is measured by the ratio of weight. So that w can be greater than 100%. Solid Air Water WT Ws Ww Wa~0 Vs Va Vw Vv VT Degree of saturation: S =Vw/Vv x 100% Saturation is measured by the ratio of volume. Moisture content: w = Ww/Ws, Ww=Vwγw Ww – weight of water, Ws – weight of solid Water content is measured by the ratio of weight. Thus, the dry unit weight γd can be approximated as: (1 )d wγ γ= − From the original form of the dry unit weight By taking the Taylor expansion and truncated at the first order term: 1d w γγ = + 2 3 4 5(1 ...) (1 ) 1d w w w w w w w γγ γ γ= = − + − + − + ≈ − + Because the moisture content w is a number always smaller than one, i.e., w<1. Relationships among S, e, w, and Gs , , 1w w v s v VS then V SV Se given V V = = = = A simple way to get Das, Equation 3.18 , 1, 1w w w w s v s s s s w s s W V eS eSw V V W V G G thus Se wG γ γ γ γ = = = = = ∴ = = ∵ When the soil is 100% saturated (S=1) we have, Equation 3.20 se wG= Relationships among γ, n, w, and Gs (1 ), 1 (1 ) s s s s w s w s s w W V G n given V n W wW wG n γ γ γ = = − = − = = − So that the dry unit weight γd is And the moist unit weight γ is (1 ) (1 ) 1 s s w d s w t W G n G n V n n γγ γ−= = = − − + (1 ) (1 ) 1 (1 ) (1 ) (1 )(1 ) t s w s w s w t t s w s w W W W G n wG n V V w G n G n w γ γγ γ γ + − + − = = = = + − = − + Example: • Determine moisture content, void ratio, porosity and degree of saturation of a soil core sample. Also determine the dry unit weight, γd Data: • Weight of soil sample = 1013g • Vol. of soil sample = 585.0cm3 • Specific Gravity, Gs = 2.65 • Dry weight of soil = 904.0g Solid Air Water Wa~0 1013.0g585.0cm3 904.0g γs =2.65 109.0g 341.1cm3 109.0cm3 243.9cm3 134.9cm3 γW =1.00 Example Volumes Weights Results • From the three phase diagram we can find: – Moisture content, w – Void ratio, e – Porosity, n – Degree of saturation, S – Dry unit weight, γd 715.0 1.341 9.243 3 3 === cm cm V Ve s v %7.41100 )(0.585 )(9.243 3 3 =×== cm cm V Vn T v %1.12100 )(904 )(109 =×== g g W Ww s w 355.1585 904 cm g V W T s d ===γ %7.44100 9.243 109 =×== v w V VS In a two-phase system, i.e., if S=100%, and we let Vs=1, we then have: eVVeV vwt ==+= since,1 Consider the not-submerged case, i.e., the two- phase system has been just put in the air: wsswssss wwww GVGVM andeVM ρρρ ρρ === == Thus, the saturated density is e Ge e Ge V MM swwsw t sw sat + + = + + = + = 1 )( 1 ρρρρ and the dry density is e G V M ws t s d + == 1 ρρ Recall that the saturated density is e Ge V MM sw t sw sat + + = + = 1 )(ρρ If we do the following wsat wsws wws w ws wsat ei e G e eGe e eGe e Ge ρρρ ρρρ ρρρρρρ −=′ ′= + − = + −−+ = + +−+ =− + + =− .,. 1 )1( 1 )1( 1 )1()( 1 )( If you have got the submerged density ρ’ and sure you know water density ρw e Ge V MM sw t sw sat + + = + = 1 )(ρρ You can calculate the saturated density ρsat.If you know ρw then you can calculate the void ratio e. if you think you can know e from the dry density ρd e G ws d + = 1 ρρ You can also calculate the submerged density ρ’ when the sample is not 100% saturated. e SeG ws + −+− =′ 1 )1()1( ρρ
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