Weight and Volume Relationships

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    Weight-Volume Relationships

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    Outline of this Lecture

    1.Density, Unit weight, andSpecific gravity (Gs)

    2.Phases in soil (a porousmedium)

    3.Three phase diagram

    4.Weight-volume relationships

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    For a general discussion we have

    density

    V=

    Weight W

    W Mg=

    Unit weightW

    V

    =

    So that

    W Mg

    gV V = = =

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    Unit weight: = gUnit weight is the product of density and

    gravity acceleration. It is the gravitational

    force caused by the mass of materialwithin a unit volume (density) in the unit of

    Newtons per cubic meter in SI system.

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    Specific Gravity (Gs)

    Specific gravity is defined as the ratio of

    unit weight (or density) of a given materialto the unit weight (or density) of water since

    s

    w w w

    gG

    g

    = = =

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    Three Phases of Soils

    Naturally occurred soils always consist of

    solid particles, water, and air, so that soilhas three phases: solid, liquid and gas.

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    Soil model

    Volume

    Solid Particles

    Voids (air or water)

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    Fully Saturated Soils (Two phase)

    Water

    Solid

    Mineral Skeleton Fully Saturated

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    Dry Soils (Two phase) [Oven Dried]

    Air

    Solid

    Dry SoilMineral Skeleton

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    Three Phase Diagram

    Solid

    Air

    WaterWT

    Ws

    Ww

    Wa~0

    Vs

    Va

    Vw

    Vv

    VT

    Weight Volume

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    Phase relationship: the phase diagram

    Wt: total weight

    Ws: weight of solid

    Ww: weight of water

    Wa: weight of air = 0

    Vt: total volume

    Vs: volume of solid

    Vw: volume of water

    Vv: volume of the void

    Solid

    Air

    WaterWT

    Ws

    Ww

    Wa~0

    Vs

    Va

    Vw

    Vv

    VT

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    Solid

    Air

    WaterWT

    Ws

    Ww

    Wa~0

    Vs

    Va

    Vw

    Vv

    VT

    Vt = Vs + Vv = Vs + Vw + Va;

    It is convenient to assume the volume of the

    solid phase is unity (1) without lose generality.

    Mt = Ms + Mw; and

    Wt = Ws + Ww, since W=Mg

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    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 enV 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.

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    Solid

    Air

    WaterWT

    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%.

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    Solid

    Air

    WaterWT

    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=VwwWw weight of water, Ws weight of solid

    Water content is measured by the ratio of weight.

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    Definition of 3 types of unit weight

    Total unit weight (moisture unit weight, wet unitweight) :

    t s w

    t t

    W W W

    V V

    +

    = =

    Dry unit weight d :

    ,sd t s d s

    t

    W V VV

    = >

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    Moisture unit weight :

    t s w

    t t

    W W W

    V V

    += =

    Solid unit weight s

    dry unit weight d

    ss

    s

    WV

    =

    ,s

    d t s d s

    t

    W

    V VV = >

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    Thus, the dry unit weight d can be approximated as:

    (1 )d w =

    From the original form of the dry unit weight

    By taking the Taylor expansion and truncated at thefirst order term:

    1d

    w

    =

    +

    2 3 4 5(1 ...) (1 )1d

    w w w w w ww

    = = + + +

    +

    Because the moisture content w is a number always

    smaller than one, i.e., w

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    Relationships amongS, e, w, and G

    s

    , , 1ww 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 vs s s s w s

    s

    W V eS eSw V VW V G G

    thus Se wG

    = = = = = =

    =

    When the soil is 100% saturated (S=1)

    we have, Equation 3.20

    se wG=

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    Relationships among, n, w, and G

    s

    (1 ), 1

    (1 )

    s s s s w s

    w s s w

    W V G n given V n

    W wW wG n

    = = =

    = = So that the dry unit weight d is

    And the moist unit weight is

    (1 )

    (1 )1

    s s wd s w

    t

    W G n

    G nV n n

    = = = +

    (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

    + + = = =

    = + = +

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    Relationships among , n, w, and Gs (cont.)

    When S=1 (fully saturated soil)

    (1 ) [ (1 ) ]1

    s w s w wsat s w

    t

    W W G n n G n nV

    + += = = +

    the moisture content w when S=1 can be expressed as

    (1 ) (1 )

    , 1

    w w

    s s w s s

    s s

    W n n ewW G n G n G

    recall Se wG thus e wG S

    = = = =

    = = =

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    Weight-Volume Relationships (Table 3.1)

    The 3rd column is a special case of the 1st column when S = 1.

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    Example:

    Determine moisture content, void ratio,

    porosity and degree of saturation of a soil

    core sample. Also determine the dry unit

    weight, d

    Data: Weight of soil sample = 1013g

    Vol. of soil sample = 585.0cm3

    Specific Gravity, Gs = 2.65

    Dry weight of soil = 904.0g

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    Solid

    Air

    Water

    Wa~0

    1013.0g585.0cm3

    904.0g

    s =2.65

    109.0g

    341.1cm3

    109.0cm3

    243.9cm3

    134.9cm3

    W =1.00

    Example

    Volumes Weights

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    Results

    From the three phase diagram we can find:

    Moisture content, w

    Void ratio, e

    Porosity, n

    Degree of saturation, S

    Dry unit weight, d

    715.01.341

    9.243

    3

    3

    ===cm

    cm

    V

    Ve

    s

    v

    %7.41100)(0.585

    )(9.2433

    3

    ===cm

    cm

    V

    Vn

    T

    v

    %1.12100)(904

    )(109===

    g

    g

    W

    Ww

    s

    w

    355.1

    585

    904

    cm

    g

    V

    W

    T

    sd ===

    %7.441009.243

    109 ===v

    w

    VVS

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    Measurement of the submerged density (or unit weight)

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    Now consider the submerged case, i.e., the two-

    phase system has been put into the water:

    wswwss

    www

    GGbuoyancyM

    andeebuoyancyM

    )1(1

    0

    ==

    ==

    Thus, the submerged density is

    e

    G

    e

    G

    V

    MM

    V

    M wsws

    t

    sw

    t

    t

    submerg +

    =+

    +

    =

    +

    =

    == 1

    )1(

    1

    )1(0

    In a two phase system i e if S=100% and we let

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    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

    ===

    ==

    Thus, the saturated density is

    e

    Ge

    e

    Ge

    V

    MM swwsw

    t

    sw

    sat +

    +=

    +

    +=

    +=

    1

    )(

    1

    and the dry density is

    e

    G

    V

    M ws

    t

    sd

    +== 1

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    Recall that the saturated density is

    e

    Ge

    V

    MM sw

    t

    swsat

    +

    +=

    +=

    1

    )(

    If we do the following

    wsat

    wsws

    wwswwswsat

    eie

    G

    e

    eGe

    e

    eGe

    e

    Ge

    =

    =

    +

    =

    +

    +=

    +

    ++=

    +

    +=

    .,.1

    )1(

    1

    )1(

    1

    )1()(

    1

    )(

    If you have got the submerged density and

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    If you have got the submerged density and

    sure you know water density w

    e

    Ge

    V

    MM sw

    t

    swsat

    +

    +=

    +=

    1

    )(

    You can calculate the saturated density sat.If youknow w then you can calculate the void ratio e. if

    you think you can know e from the dry density d

    eG ws

    d+

    =1

    You can also calculate the submerged density when the sample is not 100% saturated.

    e

    SeG ws

    +

    +=

    1

    )1()1(