Creep of Dam Concrete-j.1475-1305.2011.00818.x

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    Creep of Dam Concrete Evaluated from Laboratoryand In Situ Tests

    C. Serra, A. L. Batista and A. Tavares de Castro

    Concrete Dams Department, National Laboratory for Civil Engineering, Av. do Brasil, 101 Lisbon, Portugal

    ABSTRACT: One of the most important phenomena of the delayed behaviour of mass concrete used in dams is creep, i.e., the increase in

    deformation over time when subjected to constant stress. Although several studies concerning concrete creep were carried out throughout

    the last decades in a structural and material level, the physical and chemical phenomena are yet to be fully understood. This paper presents a

    study on the Alqueva dams concrete deformability in which a parameter evaluation was performed using the Baz ant and Panulas basic creep

    function, based on both in situ and laboratory creep test results. In the first part of the paper, the approach and material properties that

    better fit the experimental data of a dams mass concrete are presented. In the second part, the fitted function for each in situ test was

    validated using a finite element numerical model that takes into account the time-dependent behaviour, the applied stress and the monitored

    temperatures.

    KEY WORDS: concrete creep, dam concrete, FEM analysis, in situ and laboratory tests, non-linear regression models, prediction models

    NOTATION

    t time, age of concrete (days)

    t0 age of concrete at loading (days)

    J(t, t0) creep function strain (creep strain plus

    instantaneous strain) at timetcaused by a

    unit uniaxial constant stress at age t0 (GPa)1)

    E(t0) modulus of elasticity at age t0 (GPa)

    e(t, t0) total strain

    r(t0) applied stress (MPa)

    ei(t0) instantaneous strain

    ec(t, t0) creep strain

    e

    0

    (t) prescribed strainef(t, t0) specific creep (GPa

    )1)

    eesp(t, t0) specific strain (GPa

    )1)

    etotal(t, t0) experimental total strain

    eautog(t, t0) experimental autogenous strain

    fcilc t0 cylinder compressive strength at aget0 (MPa)

    fcubec t0 cube compressive strength at age t0 (MPa)

    fc,k k-day cylinder compressive strength (MPa)

    Ec,j j-day modulus of elasticity in compression (GPa)

    w/c water/cement ratio of concrete (by weight)

    a/c aggregate/cement ratio of concrete (by weight)

    s/c sand/cement ratio of concrete (by weight)

    a/g aggregate/gravel ratio of concrete (by weight)

    q unit mass of concrete (kg m)3)

    v Poissons ratio

    Introduction

    One of the most important phenomena of the delayed

    behaviour of mass concrete used in dams is creep, i.e. the

    increase in deformation over time when subjected to con-

    stant stress. Although several studies concerning concretecreep were carried out throughout the last decades in a

    structural and material level, the physical and chemical

    phenomena are yet to be fully understood. Some studies

    suggest that creep is related with displacement diffusion

    mechanism, adsorbed water movements on the surface of

    the hydrated cement, viscous deformation of the hardened

    cement, solubility increase with the applied stress and

    atomic rearrangement at the nanoscale [13].

    Concrete creep is influenced by intrinsic factors, such as

    the properties of each component, the mix proportions

    and the concreting conditions, as well as by external fac-

    tors, such as, for example, the loading age, the temperature

    and humidity levels, the intensity and type of loading

    [4, 5]. The mass concrete used in dams presents particular

    characteristics and maturity conditions over time and

    needs to be studied in detail. In addition, only a few

    studies related directly to this matter and which are based

    on long-term in situ experimental results have been pre-

    sented [69].

    The majority of the concrete creep laws currently avail-

    able were developed taking into account the results of testscarried out mainly with concrete from buildings and

    bridges [10, 11]. Throughout the last decades, the work

    developed at Northwestern University and by FIB, ACI and

    RILEM extended the experimental database to several types

    of structures, including dams, to achieve a more universal

    expression for the phenomenon of concrete creep and

    shrinkage [12]. Each creep law is normally sustained by an

    empirical or analytical formulation that determines the

    expected creep values using parameters such as the con-

    cretes ultimate compressive strength or the concretes mix

    data.

    Research carried out at the National Laboratory for Civil

    Engineering (LNEC) led to the conclusion that the creep

    function and prediction suggested by Bazant and Panula

    (BaP), known as the Double Power Law, is adequate to

    2011 Blackwell Publishing Ltd j Strain (2012) 48 , 241255 241doi: 10.1111/j.1475-1305.2011.00818.x

    An International Journal for Experimental Mechanics

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    predict dam concrete behaviour [1315]. Therefore, the

    BaP law is the basis of this study. In the first part of this

    paper, the approach and material properties that better

    fit the experimental data of a dams mass concrete are

    presented.

    In the second part of this work, it was possible to validate

    the fitted function for each in situ test using a finite-element numerical model that takes into account the time-

    dependent behaviour, the applied stress and the monitored

    temperatures.

    Determination of Creep Strains

    Definition of creep strains

    Total strain, e(t,t0), resultant of the stress, r(t0), applied at

    the aget0and kept constant untilt, can be expressed as the

    sum of an instantaneous strain, ei(t0

    ), and a creep strain,

    ec(t,t0), to which a prescribed strain, e

    0(t), can be added

    (shrinkage/expansion):

    et; t0 eit0 e

    ct; t0 e0t (1)

    The instantaneous and creep strains can be expressed as a

    function of stress, defining the creep function, J(t,t0), as the

    strain per stress unit:

    Jt; t0rt0 eit0 e

    ct; t0 (2)

    Jt; t0 1

    Et0eft; t0 (3)

    eft; t0 ect; t0

    rt0 (4)

    Measurement of creep strains

    In conventional concrete dams, the full-mixed concrete is

    made, in general, with a low cement dosage (between 150

    and 200 kg m)3) and aggregates with the maximum

    dimension of 150 mm. These characteristics are very dif-

    ferent from those of the concrete used in buildings and

    bridges.

    The accurate evaluation of the full-mixed concrete

    deformability is a key element in the dams behaviour

    assessment, whether to calibrate displacements based on

    prediction models or to interpret the behaviour using

    structural models.

    Because of the large size of the aggregates, it is difficult

    and expensive to wrap most monitoring devices and make

    sustainable test specimens in full-mixed concrete. There-

    fore, wet-screened concrete is more frequently used. This is

    obtained from the full mixed by sieving aggregates greater

    than 38 mm or 75 mm.

    Thus, as it is of interest to make in situmeasurements of

    concrete properties, creep tests are carried out on site with

    both full-mixed and wet-screened concrete giving us thepossibility of evaluating the influence of screening on the

    concrete behaviour. In the laboratory, it is only possible to

    perform experimental long-term tests with wet-screened

    concrete.

    The characterisation of the wet-screened concretes

    deformability enables the data interpretation obtained

    from the embedded devices, such as strain and stress

    meters, and allows the comparison between in situ and

    laboratory creep test results.The in situ tests are possible with full-mixed and wet-

    screened creep cells installed within the dam body, which

    allow the determination of the modulus of elasticity at any

    age and the creep strains time-history.

    Creep cells are concrete cylinders embedded in the dams

    body, subjected to the same thermohydrometric condi-

    tions as the dam body, because the top of the cell is in

    contact with the structural concrete, but isolated from the

    stress field with a steel frame that creates an overall gap

    between the cell and the dams concrete (Figure 1). The

    experimental apparatus for each type of concrete is com-

    posed by a creep cell subjected to a controlled stress, known

    as active cell, and by another cell with free deformation,

    known as non-stress cell. The first contains an embedded

    Carlson strain meter that registers the total strain varia-

    tions over time, etotal(t,t0), and the second contains another

    strain meter that measures the stress-independent strains,

    known as the autogenous strains, eautog(t,t0). As both cells

    (active and non-stress) are concreted with the same mate-

    rial, at the same time and are placed next to each other, it is

    assumed that they are subjected to the same environmental

    conditions. In addition, it is considered that the creep cells,

    embedded within the mass concrete, are saturated because

    of the water supply on the upstream face of the dam in

    contact with the reservoir.The loading system of each active creep cell is composed

    by a closed hydraulic circuit that controls the applied

    pressure on a flat jack on the base of the concrete cylinder.

    The pressure can be kept constant with the aid of a mixture

    of oil and nitrogen stored close to the creep cells (Figure 2).

    This loading system allows fast stress variations to be ap-

    plied in order to carry out modulus of elasticity tests at a

    given age and ensures constant load for long periods of

    time.

    The traditional laboratory setup is used to obtain exper-

    imental results of delayed deformations under constant

    environmental conditions. In this study, the laboratoryapparatus involved copper-sealed specimens of wet-

    screened concrete, to avoid water losses.

    The specific strains, considered to be a measurement of

    creep, are obtained by subtracting the autogenous strains,

    measured in the non-stress cell, from the total strains,

    measured in the active cell, and dividing by the applied

    stress (Equation 5) [16].

    eespt; t0 etotalt; t0 e

    autogt

    rt0 (5)

    If stress is maintained constant since the first load, one

    can compare experimental specific strains, eesp(t,t0), directly

    with theoretical specific creep, ef

    (t,t0).The complexity and variables involving the delayed

    behaviour of the concrete requires planning and controlled

    242 2011 Blackwell Publishing Ltd j Strain (2012) 48 , 241255doi: 10.1111/j.1475-1305.2011.00818.x

    Creep of Dam Concrete Evaluated from Tests : C. Serra, A. L. Batista and A. Tavares de Castro

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    concreting conditions. For the analysis of each creep cell

    and laboratory specimen results, it is necessary numerous

    related data, such as the concretes mix proportions, the

    ultimate compressive strength and the modulus of elastic-

    ity at different ages.

    Methodologies for the Creep FunctionEvaluation

    Prediction models

    Creep prediction models give a first estimation of the

    delayed deformations using required measured concrete

    properties. These models are useful in the design stage and

    when there are no specific test results available. In impor-

    tant structures, such as large dams, specific and extensive

    tests are commonly carried out to determine the concretes

    compressive strength, modulus of elasticity and creepstrains, although major direct and delayed costs [17].

    The prediction models are based on functions that

    translate the physical phenomenon. The function param-

    eters, usually obtained from known material properties

    and, whenever possible, adjusted to experimental results,

    allow creep strains estimation, considering established

    hypothesis.

    There are several formulations for the prediction of the

    delayed deformations [11, 14, 1820]. However, studies

    carried out at the National Laboratory for Civil Engineering

    (LNEC) since the 1980s [4, 21, 22] have shown that the

    prediction model proposed by BaP between 1975 and 1979

    [1315], known as the Double-Power Law, provides a good

    fit to the general monitoring results of the Portuguese

    concrete dams [4].

    The advantage of this type of function is the fact that

    creep is computed as the sum of both basic and drying

    creep. The basic creep holds the maturity process by

    including a power of the age at loading, t0, and a power of

    the time since loading, t) t0 (Equation 6).

    Jt; t0 1

    E0u1E0

    tm0 att0n

    (6)

    whereE0, u1, m, a and n are given parameters.

    The prediction of the static modulus of elasticity is

    considered to be the inverse of the creep compliance con-

    sidering 0.1 days as the loading time (Equation 7) [15].

    Figure 2: View of the non-embedded devices of the creep cellloading system

    Figure 1: Representation of the active and non-stress creep cells for both full-mixed and wet-screened concrete

    2011 Blackwell Publishing Ltd j Strain (2012) 48 , 241255 243doi: 10.1111/j.1475-1305.2011.00818.x

    C. Serra, A. L. Batista and A. Tavares de Castro : Creep of Dam Concrete Evaluated from Tests

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    1

    Et0

    1

    E0u1E0

    10ntm0 a (7)

    The parameters can be obtained by two different empir-

    ical formulations. The first relies on the 28-day ultimate

    concrete compressive strength, fc,28, and on the concretes

    mix data (Equations 815) [15].

    u1 103n

    228m a (8)

    a 1

    40w=c (9)

    m 0:28 47:541f2c;28 (10)

    n 0:12 0;07x6

    5130x6 sex >0

    0:12 sex 0

    (11)

    x 2;1 a=c

    s=c1;4 5;523 103f1;5c;28

    w

    c 1=3 a

    g 2;2

    " #a1 4 (12)

    a11:0 cementtypeI ouII general0:93 cementtype III fast hardening1:05 cementtypeIV low hydration heat

    8