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    Development of sustainable landfill practices

    and engineering landfill technology

    Final report to the Engineering and Physical Sciences Research Council

    (Grant reference GR/L 16149)

    W Powrie

    A P HudsonR P Beaven

    Department of Civil & Environmental Engineering, University of Southampton, Highfield, SouthamptonSO17 1BJ

    February, 2000

    Note: the format of this report is specified by EPSRC. The main body of the text is limited in length to six

    pages of typescript. Further details may be found in the papers listed in Appendix B, copies of which are

    available on request from Professor W Powrie.

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    Research Grant Title: Development of sustainable landfill practices and engineered landfill technology

    (GR/L 16149)

    Investigators and Institutions: W Powrie, A P Hudson, R P Beaven, C J Banks, D Montagnani and T W Tanton,

    Department of Civil and Environmental Engineering, University of Southampton; and J P Robinson, Queen Mary

    and Westfield College. Project carried out with additional funding from and in collaboration with Cleanaway Ltd.

    Summary: In recent years, the driving principle of landfill management has been to prevent saturation of the waste

    to minimize the likelihood of leachate leaking into the surrounding ground. This has resulted in very slow rates of

    waste degradation, with projected stabilization times of the order of hundreds of years. Degradation could in

    principle be accelerated by circulating fluids through the waste in a controlled manner, and operating the landfill as

    an engineered wet bioreactor. This approach is more consistent with the aims of a sustainable waste management

    policy than the entombment approach, which leaves landfilled wastes in a potentially polluting state for many

    generations.

    One of the main uncertainties concerning the practicality of operating a landfill as a controlled bioreactor is the

    hydraulic conductivity of the waste, because this governs the ease with which fluids may be introduced into and

    extracted from the landfill. The aim of the research described in this report was to develop an understanding of the

    factors controlling the hydraulic conductivity of landfilled wastes, in the context of the design and operation of a

    landfill as an engineered flushing bioreactor.The research consisted of three components:

    large scale experiments on samples of wastes, carried out at Cleanaway Ltds Pitsea landfill site in a purpose-

    built compression cell;

    laboratory studies to investigate (a) the impact of leachate/liquid recirculation on waste degradation rates, (b)

    moisture content suction relationships for certain types of waste, and (c) the feasibility of monitoring

    changes in geotechnical and hydraulic properties, settlement and gas generation rates in samples of wastes

    during leachate/liquid recirculation under constant applied stress; and

    the development of simple models to enable the application of the results of the experimental work to the

    sustainable operation of landfills.

    A key factual output of the research has been the quantification of relationships between the drainable porosity

    and vertical stress, and between hydraulic conductivity and vertical stress, for samples of processed, unprocessed

    and aged household waste. On the basis of these data, and using simple analytical models developed to enable

    their application to problems in landfill operation, the following conclusions can be made.

    At depth, most wastes are likely to be approaching saturation even if they are free to drain under gravity.

    Although some differences in hydraulic conductivity between processed, unprocessed and aged household

    wastes were apparent, these are generally insignificant in comparison with the orders of magnitude change in

    hydraulic conductivity that results from waste compression.

    On unloading, very little of the deformation due to loading was recovered, and the hydraulic conductivity

    remained substantially unchanged. Thus the hydraulic conductivity of a waste is governed by the maximum

    equivalent vertical stress to which the waste has been subjected, so that the stress history or the density of the

    waste must be considered when assessing its hydrogeological and geotechnical properties.

    During compression, waste develops a layered structure. This results in a degree of anisotropy of hydraulic

    conductivity (expressed as the ratio Kh/Kv) that increases with increasing applied stress.

    Provided that the dependence of hydraulic conductivity on vertical stress and stress history is taken into

    account, calculations suggest that vertical infiltration rates comparable with achieving stabilization of the wastewithin a timescale of one generation can be achieved. Precompaction of the waste to densities greater than 0.9 -

    1.1 t/m3, or placement of loose waste unsaturated to a depth in excess of about 40 m prior to saturation, would

    both prevent the required infiltration rate from being realised.

    Analyses of pumped vertical wells using a stress dependent hydraulic conductivity suggest that there will be

    little increase in flowrate for increases in drawdown in excess of about 33% of the initial saturated depth.

    Preliminary tests have demonstrated the importance of the interaction between gassing and leachate flow in

    terms of the pore volume available for liquid flow, and suggest that changes in gas production rate could affect

    the apparent leachate level measured in the field. This is a subject requiring further research.

    EPSRC grant and duration For further information please contact

    231,226 over 36 months Professor W Powrie, Department of Civil & Environmental

    plus project studentship Engineering, University of Southampton SO17 1BJ

    (tel. 023 80593214; fax 023 80677519; e-mail [email protected])

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    1

    1. BACKGROUND AND OBJECTIVES

    1.1 Background

    In recent years, the driving principle of landfill management has been to prevent saturation of the waste to

    minimize the likelihood of leachate leaking into the surrounding ground. This has resulted in very slow rates of

    waste degradation, with projected stabilization times of the order of hundreds of years (e.g. Knox, 1990).

    Degradation could in principle be accelerated by circulating fluids through the waste in a controlled manner, andoperating the landfill as an engineered wet bioreactor. This concept, which is espoused by Waste Management

    Paper 26B (DoE, 1995), offers significant economic and environmental benefits and is more consistent with the

    aims of a sustainable waste management policy than the entombment approach, which leaves landfilled wastes in

    a potentially polluting state for many generations.

    One of the main uncertainties concerning the practicality of operating a landfill as a controlled bioreactor is

    the hydraulic conductivity of the waste, because this governs the ease with which fluids may be introduced into

    and extracted from the landfill. This was the issue addressed by the research described in this report.

    1.2 Aims and objectives

    The aim of the research was to develop an understanding of the factors controlling the hydraulic conductivity of

    landfilled wastes, in the context of the design and operation of a landfill as an engineered flushing bioreactor. As

    stated in the original case for support, these included the effects of waste composition, overburden pressure,microbial activity, degradation and two phase flow (gassing). However, a budget reduction of 100,000 from the

    329,927 initially requested necessitated a reduction in the scope of the research. In the light of guidance

    received from the Waste and Pollution Management Programme Management Committee, the work on the effect

    of waste composition was deleted from the programme, and the work on the effects of waste degradation and

    gassing (two -phase flow) scaled down considerably. The objectives of the proposed research were revised from

    those given in the original case for support. The revised objectives were

    to quantify the effects of overburden pressure on the mechanical and hydraulic properties of different types

    of waste, and

    to carry out a preliminary assessment of the effects of microbial activity on the mechanical and hydraulic

    properties of wastes

    in the context of the operation of a landfill as an engineered wet bioreactor, as stated in a letter from Professor W

    Powrie (UoS) to Dr M Partridge (EPSRC) dated 18 April 1996.

    2. PROGRAMME MANAGEMENT

    In addition to the EPSRC grant, the project was funded by a donation of 150,000 from Cleanaway Ltd under the

    Landfill Tax Credit Scheme. The research may conveniently be divided into three components:

    large scale experiments on samples of wastes, carried out at Cleanaway Ltds Pitsea landfill site in a purpose-

    built compression cell;

    laboratory studies to investigate (a) the impact of leachate/liquid recirculation on waste degradation rates, (b)

    moisture content suction relationships for certain types of waste, and (c) the feasibility of monitoring

    changes in geotechnical and hydraulic properties, settlement and gas generation rates in samples of wastes

    during leachate/liquid recirculation under constant applied stress; and

    the development of simple models to enable the application of the results of the experimental work to the

    sustainable operation of landfills.

    The work using the Pitsea compression cell was carried out by Andrew Hudson, a Research Assistant funded by

    the EPSRC grant, under the supervision of Dr R P Beaven (Senior Research Fellow funded from the grant) and

    Professor W Powrie (Principal Investigator). The laboratory studies were carried out by (a) Daniele Montagnani,

    an EPSRC-funded project research student associated with this grant (supervised by Dr C J Banks); (b) Mansoor

    Imam, a research student funded by the Faculty of Engineering and Applied Science and the Department of Civil

    and Environmental Engineering at the University of Southampton (supervised by Dr D J Richards); and (c) Lewis

    Parker, a research student at QMW (supervised by Professor J K White and Dr J P Robinson). The development

    of models for the application of the results to sustainable landfill practice was carried out by Professor W Powrie

    and Dr R P Beaven.

    The project was overseen by a steering group comprising:

    Professor W Powrie, University of Southampton; Dr R P Beaven, University of Southampton;

    Dr C J Banks, University of Southampton; Dr J P Robinson, QMW;

    Dr L de Rome, ETSU (for EPSRC); and Mr M J Dyer, Cleanaway Ltd.

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    Additional input and advice was provided on an ad hoc basis by Professors T W Tanton and J B Joseph.

    Early dissemination of the results has been achieved by means of

    papers published in the Sardinia International Landfill Conference, 1999 and the Proceedings of the

    Institution of Civil Engineers special issue on Landfill Engineering (October 1999);

    an article in Waste Management, (November 1998); presentations at seminars at the Nottingham Trent University (September 1998), University College London

    (January 1999), the Institution of Civil Engineers (ICE), London (November 1999), the ICE South Wales

    Geotechnical Group, Swansea (November 1999), the University of Southampton (December 1999), and WRc

    leachate management workshops; and

    Dr Beaven and Professor Powries membership of the Institution of Wastes Management Working Group on

    Sustainable Landfill, which published its report in Spring 1999

    A full list of papers and reports published to date is given in Appendix B.

    3. DESCRIPTION OF THE RESEARCH

    3.1 The Pitsea compression cell: modifications, waste testing and new experimental techniques

    Most of the experimental research was carried out using the Pitsea compression cell. This is a purpose built

    apparatus for determining the hydrogeological and geotechnical properties of 2 m dia. samples of waste atstresses up to 600 kPa (Figure 1). The cell was originally used in research sponsored by the Waste Technical

    Division of the Department of the Environment and Cleanaway Ltd. To enhance the testing capabilities and

    improve the quality of the data, a number of major modifications were made to the cell and new testing protocols

    were developed as part of this research. New techniques for analysing experimental data from the Pitsea

    compression cell have also been developed, and applied to the results of both this research and earlier tests

    (Section 3.1).

    Two new wastes were tested in the Pitsea compression cell. Waste AG2 was a 20 year old (predominantly

    household) waste excavated from a landfill (Table 1). Waste DN1 was household waste that had been processed

    using the DANO technique (Table 2); it was selected as an example of a processed waste that had previously

    been used in field scale research in the Mid-Auchencarroch landfill (Wingfield-Hayes et al, 1997). Initially, it had

    been hoped that a t least one other waste type would have been tested in the Pitsea compression cell. However, it

    was decided during the course of the research to investigate the properties of the wastes in unloading as well as

    loading, which increased considerably the duration of the testing programme for each waste. Data from earlier

    tests on crude household waste (DM2 and DM3 -Table 3), pulverised waste (PV1 and PV2 -Table 4) and an aged

    waste (AG1 -Table 5) were re-analysed and used together with the new results to develop theories and models

    concerning sustainable landfill (Section 3.3).

    3.1.1 Building Enclosure

    An improved working environment and more controlled test conditions have been created by the construction of

    an enclosure to the building (Figure 2). This was financed by a contribution from Cleanaway Ltd through the

    landfill tax credit system.

    3.1.2 Modifications to allow horizontal hydraulic conductivity to be measured

    To measure horizontal hydraulic conductivity in the compression cell, it was necessary to induce horizontal flow

    across the samples. This required the addition of eleven inlet ports and eleven diametrically opposite outlet portsto the compression cell wall. Extra piezometer monitoring ports were also added. To monitor the individual flow

    rates through each of the inlet ports, eleven small header tanks were constructed and mounted on the header tank

    scaffold tower (Figure 3). Inflatable seals were added around the perimeter of the top platen to prevent leakage

    through the clearance gap against the cylinder wall.

    3.1.3 Modifications to monitor effects of degradation

    The construction of landfill gas collection facilities on the Pitsea compression cell and the provision of a sensitive

    load cell weighing system has allowed a preliminary assessment to be made of the effect of gas on the

    hydrogeological properties of waste, in particular on the drainable porosity and hydraulic conductivity. The

    displacement of gas from the waste by liquid flow was measured for a range of flow rates in upward, downward

    and horizontal flow.

    3.1.4 Measurement of differential waste compression within the cell

    Load is applied to the upper surface of waste samples in the compression cell through a hydraulically operated

    platen. Sidewall friction between the cylinder walls and the waste causes a reduction with depth in the vertical

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    stress transmitted to the waste. This may result in differential compression of the sample, and hence a variation in

    hydrogeological properties with depth. A magnetic ring extensometer has been successfully installed and used to

    measure the pattern of waste compression within the cell (Figures 4 & 5).

    3.1.5 Load Cells

    Accurate measurement of the weight of samples is necessary for density calculations, and for monitoring water

    and gas content. The existing equipment was unsatisfactory and had to be replaced.

    3.1.6 Data interpretation and analysis of results from Pitsea compression cell

    A correction for the effect of sidewall friction has been developed (Powrie and Beaven, 1999), and data are now

    reported as functions of the average transmitted vertical stress.

    As direct measurement of the horizontal hydraulic conductivity of waste samples is not possible owing to the

    geometry of the compression cell, the USGS three dimensional groundwater flow model MODFLOW (in

    combination with Groundwater Vistas) was used to model the flow regime (e.g. Figure 6). Measured flow rates

    and leachate pressure heads within the waste were matched with computer analyses to obtain the horizontal

    hydraulic conductivity of samples at different vertical stresses (Hudson, Beaven and Powrie, 1999).

    3.2 Laboratory based tests

    3.2.1 Unsaturated suction curve characterisationWaste moisture characteristic curves were determined for samples of Dano processed waste using a filter paper

    contact method (ASTM D5298-92).

    3.2.2 Effect of flushing rate on waste degradation

    The benefits of leachate treatment, either within or external to the landfill, and the effect of leachate recirculation

    or flushing rate on optimizing waste degradation were assessed in 1-litre, 21 day batch laboratory experiments on

    the organic fraction of municipal solid waste (OFMSW). The initial biological methane potential (BMP) was used

    as a benchmark against which to assess the degradation of the waste. The effects of hydraulic retention time

    (experimental range 80 to 240 hours) and flushing medium (tap water, aerobically treated leachate and

    anaerobically treated leachate) on degradation were assessed by monitoring the change in total and volatile

    solids, the organic content (TOC, TON, VFA) of the flushing liquor and the quantity and composition of gas

    production. Larger scale experiments, to confirm the findings of the batch experiments, were carried out in 30-litre

    static bed upflow lysimeters packed with OFMSW and inert pore rings, which increased the porosity of the waste

    material allowing shorter hydraulic retention times (Figure 7).

    3.2.3 Effect of degradation on properties of degrading solid waste

    A prototype laboratory scale anaerobic refuse digester has b een built to measure the effects of waste degradation

    on the physical and hydrogeological properties of refuse whilst subjected to vertical effective stresses typical of

    those encountered in a landfill (Figure 8).

    The reactor chamber is an acrylic cylinder, 476mm in diameter and 900mm high providing a capacity of 160

    litres. The chamber is placed within an Eland Engineering T413/2 loading frame, where it is subjected to a constant

    vertical stress while liquid is circulated through the waste. Instrumentation is incorporated to measure the

    following:

    pore water pressures and leachate recirculation rates reactor chamber temperature

    influent/effluent leachate chemistry gas production and composition waste density and settlement hydraulic conductivity

    drainable porosity

    The successful functioning of the cell and monitoring systems, and the feasibility of assessing the effects of

    degradation in this way, have been demonstrated using a 20 year old sample of waste (AG2).

    3.3 Development and application of models for flow in landfills

    To start applying the results of the research to landfill operations, a number of analytical and numerical flow

    models taking into account the variation of hydraulic conductivity with effective stress have been developed:

    one dimensional vertical flow or infiltration was modelled using a finite difference method, with density and

    hydraulic conductivity dependent on the effective stress (Powrie and Beaven, 1999),

    closed form analytical solutions were derived relating the discharge from a well to the drawdown in

    unconfined and confined aquifers where the hydraulic conductivity depends on the effective stress (Figure 9:

    Powrie and Beaven, 1999), and

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    the USGS three dimensional ground water flow model MODFLOW was modified to incorporate hydraulic

    conductivities that vary with effective stress. The model was verified against the simpler analytical and finite

    difference solutions above. It was then used to simulate more complex leachate flow problems, including the

    performance of a grid of leachate injection and abstraction wells (Figure 10: Beaven and Powrie, 1999).

    4. MAJOR RESULTS AND FINDINGS

    4.1 Waste density and water contentFigure 11 shows the dry density as a function of effective stress for the different wastes tested. The sample with

    the highest dry density was the 20 year old aged waste excavated from a landfill site. This is consistent with the

    large proportion of soil type material (represented by the

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    load, or from increases in the pore water pressure. However, no significant changes in drainable porosity or

    hydraulic conductivity were detected when the effective stress was reduced. The implication of this is that fluid

    flow in landfills will be predominantly controlled by the maximum previous effective stress to which the waste has

    been subjected. Any loading process, such as placement of the waste in an unsaturated state or dewatering by

    pumping from a vertical well, will probably cause an irreversible reduction in hydraulic conductivity.

    4.5 Waste particle density and effective stress theoryThe results of the tests undertaken in the compression cell suggest that the waste particles undergo significant

    changes in density as the overburden stress is increased (Table 8). This is in contrast to some of the theories

    used in conventional soil mechanics, in which the particles are assumed to be incompressible. On the basis of the

    data in Table 8 for raw household refuse at 120 kPa and above, the effective stress for calculations of volume

    change would be ' = - A.uw, where A lies in the range 0.19 to 0.57 (Powrie, Beaven and Harkness, 1999). In

    general terms, the applicability of the principle of effective stress to landfilled wastes remains a subject requiring

    further research.

    4.6 Unsaturated waste characteristics

    Figure 19 shows the relationship between suction and water content for the Dano processed waste at an average

    bulk density of 700 kg/m3. These data will be essential to any future modelling of flow in the unsaturated zone.

    4.7 Effect of flushing rate on waste degradation

    The batch scale experiments on the degradation of OFMSW showed that solids destruction increased as the

    flushing rate increased and HRT reduced (Figure 20). The greatest amount of solid destruction were achieved

    with a tap water flush, and the lowest with anaerobically treated leachate. The formation of volatile fatty acid

    (VFA) was stimulated by higher flushing rates and is a reflection of the greater solids destruction. Gas production

    from the batch reactors depended on the available soluble substrate concentration, and is shown for the various

    recirculation systems in Figure 21 (a-d). Gas production in reactors operating at reduced flushing rates (HRTs of

    240 and 504 hours) was impeded due to the inhibition of substrate hydrolysis as a result of an accumulation of

    VFA and/or a lowered pH. Gas production was also impeded in reactors operating at high flushing rates with

    deionised water, due to the washing out of essential ions and poor buffering.

    The larger scale experiments generally confirmed the findings of the smaller experiments. A summary of typical

    results is given in Table 9, which indicates a substantial increase in degradation on flushing with tap water,

    although there was no additional benefit from increasing the flushing rate to give a hydraulic retention time of

    less than 4 days. Flushing with untreated leachate significantly reduced the amount of solids destruction.

    The work has increased our understanding of how the flushing medium influences degradation, and has

    shown quite clearly the beneficial effects of VFA removal in a leachate recirculation system.

    5. SIGNIFICANCE OF RESULTS FOR ENGINEERING PRACTICE

    5.1 Maximum vertical infiltration rates through landfills

    A key constraint on the viability of the flushing bioreactor as a sustainable landfill is the rate at which flushing

    can take place. A one dimensional flow model incorporating empirical relations between waste density and

    effective stress (e.g. Figure 13) and hydraulic conductivity and effective stress (e.g. Figure 17) was developed to

    examine maximum infiltration rates through landfills of various depths with different initial waste densities (Powrie

    and Beaven, 1999). These flow rates were related to the minimum required to flush the pollution load from landfills

    over a 30 year period, which is consistent with the definition of a sustainable landfill as one that is approachingequilibrium with the surrounding environment within a period of one generation from cessation of landfilling

    activities (e.g. IWM, 1999). Greater flushing rates are achieved through saturated than unsaturated waste. Landfill

    depths would need to be less than approximately 20 m to achieve the necessary flushing rates through

    unsaturated wastes and less than approximately 40 m through saturated waste, if it is assumed that hydraulic

    conductivity is governed by the effective stresses applied during placement of the waste in an unsaturated state.

    If the waste is placed saturated, there is virtually no limit on landfill depth to achieve the required flushing rate

    (Figure 22). Pre-compaction of waste at the tipping face can also affect possible flushing rates (Figure 23): in

    general waste should not be compacted to densities greater than between 0.9 and 1.1 t/m3.

    5.2 Flow to a pumped leachate well

    Flowrate-drawdown curves for pumped wells in confined and unconfined aquifers whose hydraulic conductivity

    varies with effective stress are shown in Figure 24. The unconfined aquifer analysis (Figure 24b) is more

    representative of field conditions at many landfills. The specific capacity (i.e. the flow rate per unit drawdown)

    decreases with increasing drawdown. The flowrate increases with drawdown, but there is little increase in flowrate

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    for increases in drawdown in excess of about 33% of the initial saturated depth. This is an important result that

    has significant operational implications for the pumping of leachate from wells on landfills.

    5.3 Leachate flushing using a well field

    MODFLOW was used to investigate the feasibility of using vertical wells to flush waste horizontally in a 30 metre

    deep landfill with a 20 metre confined saturated zone. With a grid spacing of 20 metres, the model (Figure 25)

    calculated a steady state pumping and injection rate of 4.3 m3/day based on a fixed hydraulic conductivity profilerelated to the stress distribution in unsaturated waste. This pumping rate is theoretically sufficient to flush and

    remove contaminants from all areas of the waste between the wells in approximately 30 years. The flow or flushing

    rate at the top of the saturated layer is approximately 20 times the rate at the bottom (Figure 26). If K h is increased

    relative to Kv (Figure 18) then the pumping rate is increased and the ratio of the flowrates at the top and bottom is

    reduced to 8. Nevertheless, flushing strategies involving vertical wells will probably require the targeting by

    discrete well response zones of different horizons in the waste.

    6. PRINCIPAL CONCLUSIONS

    Relationships between the drainable porosity and vertical stress have been quantified for a number of

    wastes. At depth, most wastes are likely to be approaching saturation even if free to drain under gravity.

    Relationships between hydraulic conductivity and vertical stress in first compression have also been

    determined. Although some differences in hydraulic conductivity between processed, unprocessed and agedhousehold wastes were apparent, these are generally insignificant in comparison with the orders of

    magnitude change in hydraulic conductivity that results from waste compression.

    On unloading, very little of the deformation caused by loading was recovered, and the hydraulic conductivity

    and drainable porosity remained substantially unchanged. This suggests that the hydraulic conductivity of a

    waste is governed by the maximum equivalent vertical stress to which the waste has been subjected, so that

    the stress history or the density of the waste must be considered when assessing its hydrogeological and

    geotechnical properties.

    During compression, waste develops a layered structure which results in an anisotropy of hydraulic

    conductivity. The degree of anisotropy, expressed as the ratio Kh/Kv, increases with increasing applied

    stress.

    Provided that the dependence of hydraulic conductivity on vertical stress and stress history is taken into

    account, calculations suggest that vertical infiltration rates comparable with achieving stabilization of the

    waste within a timescale of one generation can be achieved. Precompaction of the waste to densities greater

    than 0.9 - 1.1 t/m3, or placement of loose waste unsaturated to a depth in excess of about 40 m prior to

    saturation, would both prevent the required infiltration rate from being achieved.

    Analyses of pumped vertical wells using a stress dependent hydraulic conductivity suggest t hat there will be

    little increase in flowrate for increases in drawdown in excess of about 33% of the initial saturated depth. If

    arrays of vertical wells are used for horizontal flushing, the tendency for preferential flow through the upper

    saturated layers will need to be addressed.

    Preliminary tests have demonstrated the potential importance of the interaction between gassing and

    leachate flow in terms of the pore volume available for liquid flow, and suggest that changes in gas

    production rate could affect the apparent leachate level measured in the field. This is a subject requiring

    further research.

    7. ACKNOWLEDGEMENTSThe research summarized in this report was carried out with the support of the Engineering and Physical Sciences

    Research Council (EPSRC), with an additional financial contribution from Cleanaway Ltd.

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    Figure 1 Pitsea compression cell prior to modifications Figure 2 New enclosure to Pitsea compression cell

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    Figure 3 Configuration of horizontal hydraulic conductivity tests

    Supply Tank

    Header tanks

    Cylinder

    Gravel layer

    Isolated ports

    Seal

    Bottom platen

    Inlet Ports

    Inlet Valves

    Gravel layerFlow

    outlets (isolated)

    Outlets

    Piezometer tubesinserted in sampleat various positions

    Piezometrichead

    New Seals

    Top platen

    Top platenoutlets

    (isolated)

    Tomeasuring

    cylinder

    Waste Sample

    Figure 4 Magnet and extensometer method of measuring sample movement

    3 way valve mounted on top for either:

    * Outflow to reservoir tank

    * Outflow to gas collection tank

    * Inflow from header tanks

    * Isolated

    Pointer fixed to framework

    Plastic tube - 3m long

    Bottom of tube sealed and

    resting on bottom platen

    Water & gas tight seal

    Unclamped to allow

    platen movement

    Gravel layer - for water

    distribution or removal

    Dividing Ring - 1400mm dia x 150mm deep

    Creates an inner and outer core in the

    sample for assessing preferential flow paths

    Valve stems

    Part of strengthening framework

    Extensometer - lowered into

    tube. Magnet position indicated

    with buzzer and warning light

    Magnet & plate

    Sample movement causes

    magnet to slide on tube

    Waste sample

    - forced downwards

    by applied load

    Waste cylinder (ID2000mm)

    - fixed position

    Inflatable seals(3 off)

    Clearance Gap (5mm nominal)

    rings for seals

    Graduated tape

    12 holes through top platen

    with flanged extension tubes

    Top Platen - Dia 1990mm

    Connected to hydraulic rams

    for application of load to waste

    Fabricated retaining

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    Figure 5 Magnet displacement in waste DN1 between 0 and 87kPa illustrating uniform compression

    0

    100

    200

    300

    400

    500

    600

    700

    800

    0 200 400 600 800 1000 1200 1400 1600

    Elevation above base of waste (mm)

    Downnrddisplacementrelativetopositionat0kPa(mm)

    Magnet positions end of 40kPa Magnet positions - end of 87kPa

    Uniform compression (40kPa) Uniform compression (87kPa)

    Figure 6 Typical MODFLOW simulation to determine KhWest EastCross-Section along Row 29

    470

    470

    490

    490

    510

    510

    510

    510

    530

    53

    0

    530

    550

    550

    570

    570

    590

    590

    610

    6306

    50

    670

    Top Gravel

    layer

    Outlet Port

    constant head

    cells

    Pressure head contours (cm AD):

    asymmetry reflecting lower

    hydraulic conductivity at the top

    of the waste

    Bottom Gravel

    layer

    No flow squares

    (light grey) denoting

    outside wall of

    cylinder

    Constant head squares

    simulating outflow

    through the

    bottom platen.

    Inlet Port

    constant head

    cells

    Constant head squares

    simulating outflow

    through the

    upper platen.

    Model calibrated against measured input andoutput flow rates and hea

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    Figure 7 Process diagram for ... dan's work

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    Figure 8 Anaerobic consolidation reactor

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    Figure 9 Ideal (a) confined and (b) unconfined aquifer analyses of flow to a well where K=f(')

    h w zh

    H , D ( = 2 0 m )

    Flow to wel l

    b ) U n c o n f i n e d

    a ) C o n f i n e d

    h w

    zh D ( = 1 0 m )

    D (=20m)

    F low to we l l

    Con f in ing laye r

    r w r0

    In bo th ana lyses ln ( ro /r w) =8 an d t he un it we ig ht of s at ur at ed an d un s at ur at ed

    w a s t e = 1 1 k N / m 3

    1

    2

    1

    2

    (1+)D (=30m)

    H ( = 2 0 m )

    Figure 10 MODFLOW grid design to simulate operation of injection and abstraction wells

    5 1 0 1 5 2 0 2 5 3 0 3 5

    35

    30

    25

    20

    15

    10

    5

    Elevat ion

    P lan

    C o n s t a n t h e a d b o u n d a r y c e l l s

    ( a t e a c h c o r n e r o f t h e g r i d )

    r e p r e s e n t h e a d i n 1 / 4 o f e i t h e r

    p u m p e d o r i n j e c t i o n w e l l

    N o f l o w b o u n d a r y c e l l s1

    2

    1 1

    2 1

    West East

    Layer

    Nu mb e r s

    W e l l 2

    W e l l 1

    W e l l 3

    W e l l 4

    C o l u m n s

    R o w s

    20m

    10m

    20.2m

    20.2m

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    Figure 11 Dry density vs effective stress

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 100 200 300 400 500

    Average effective stress (kPa)

    Drydensity(t/m3)

    Household waste DM3 Household waste DM2 Processed waste PV1

    Processed waste PV2 Aged waste AG1 Aged waste AG2

    Dano waste DN1

    Figure 12 Water content at field capacity of crude household waste vs effective stress

    40

    50

    60

    70

    80

    90

    100

    110

    0 100 200 300 400

    Av. Stress (kPa)

    WCdry(%)

    Household waste 3 at Field Capacity Original Water Content

    Absorptive

    Capacity

    (between lines)

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    Figure 13 Average density of Household Waste vs effective stress

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    1.1

    1.2

    0 100 200 300 400 500 600

    Av. vertical stress in waste (kPa)

    Density(t/m3)

    Dry density of DM2 and DM3 Density at Field CapacitySaturated density Density at original water content

    Power (Density at Field Capacity)Power (Density at original water content)

    dry = 0.1554.(') 0.248

    FC= 0.448.(') 0.1563

    sat = 0.6691.(') 0.0899

    = 0.236.(') 0.248

    B u l k d e n s i t y r a n g e o f

    w a s t e s

    unsatura ted

    Figure 14 Average drainable porosity vs effective stress

    0

    5

    10

    15

    20

    25

    0 100 200 300 400 500

    Average effective stress (kPa)

    Drainab

    leporosity(%)

    Household waste DM3 Household waste DM2 Processed waste PV1

    Processed waste PV2 Aged waste AG1 Aged waste AG2

    Dano waste DN1

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    Figure 15 Effect of waste degradation and landfill gas production on the proportion of leachate occupying

    drainable porosity voids

    Figure 16 Effect of leachate movement on leachate and gas occupation of drainable voids in waste DN1 at 40

    kPa: upward flushing

    0

    1 00

    2 00

    3 00

    4 00

    5 00

    6 00

    7 00

    8 00

    0 2 4 6 8 10 12

    Time(days )

    Volumeofgasinwaste(litres)

    0

    1000

    2000

    3000

    4000

    5000

    6000

    7000

    Accumulatedgasvolume(litres)

    Volume of gas in waste (based on load ce l l readings and vo lume of leachate d isp laced)

    Volume of gas vented to a tmosphere by sample

    Leachate occup ied

    drainable porosity = 5%

    Leachate occup ieddrainable porosity = 0%

    Leachate occup ied

    drainable porosity =10%

    Leachate occup ied

    drainable porosity = 15%

    Leachate f lushing

    event at Q=1.5 l /s

    Leachate f lushing

    event at Q=1.5 l /s

    Leachate f lushing

    event at Q=1.5 l /s

    0

    2

    4

    6

    8

    10

    12

    14

    16

    0 0 . 0 005 0 . 001 0 . 00 15 0 . 002 0 . 0 025 0 . 00 3 0 . 0 035 0 . 00 4 0 . 004 5

    A v e r a g e l i n e a r f l o w v e l o c i ty b a s e d o n l i q u i d f i l l e d v o i d s (m / s )

    Leachateoccupieddrainablevoids(%)

    Le ac hat e oc cupi ed dr ai nabl e v oi ds D ra ina bl e po ro si ty (10 0% lea ch at e s at ur at io n)

    Increas ing t ime

    of f lush ing

    Increas ing t ime

    of f lush ing

    Increas ing t ime

    of f lush ing

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    Figure 17 Hydraulic conductivity vs stress

    1.E-09

    1.E-08

    1.E-07

    1.E-06

    1.E-05

    1.E-04

    1.E-03

    10.0 100.0 1000.0

    Hydraulicconductivity(m/s)

    D M 3 P V 1 A G 1 A G 2

    D N 1 Ser i es2 Ser i es4

    Av. vertical stress (kPa)

    K (m/s) = 10(') -3.1

    (approx best fit line)

    K (m/s) = 80(')-3.63

    (approx fit based on

    worst case hydraulic

    conductivity)

    Figure 18 Anisotropy in hydraulic conductivity

    1

    2

    3

    4

    5

    0 100 200 300 400 500 600Applied Stress (kPa)

    Kh

    /Kv

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    Figure 19 Dano waste moisture characteristic curve

    Figure 20 OFMSW total solids destruction in 1 litre anaerobic digestion vessels operating variable

    hydraulic retention times and flushing with different liquors, operated over a 21 day time period.

    1 0 0 0

    1 0 0 0 0

    1 0 0 0 0 0

    0 1 0 2 0 3 0 4 0 5 0 6 0

    Moisture content (w) %

    Dry Weight basis

    Suction(kPa)

    0.00

    10.00

    20.00

    30.00

    40.00

    50.00

    60.00

    0 100 200 300 400 500 600

    Hydrau l ic Retent ion T ime (hrs)

    Solids

    destruction(%)

    tap water aerob ic trea tment anaerob ic trea tment de- ion ized water

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    Figure 21 Cumulative biogas production for anaerobic bioreactors with hydraulic retention time of

    a) 80 hrs; b) 120 hrs; c) 240 hrs; and 504 hrs. Flush liquors: tap water; de-ionized water; leachate after secondary anaerobic treatment; leachate after

    secondary aerobic treatment

    a) b)

    0

    1000

    2000

    3000

    4000

    5000

    6000

    0.00 100.00 200.00 300.00 400.00 500.00 600.00

    time (hrs)

    biogasproduced(ml

    Anaerobic Secondary Treatment Deionized Water Flush Aerobic Secondary Treatment Tap Water Flush

    c) d)

    0

    1000

    2000

    3000

    4000

    5000

    6000

    0.00 100.00 200.00 300.00 400.00 500.00 600.00

    time (hrs)

    biogas(ml)

    Anaerobic Secondary Treatment Deionized Water Flush Aerobic Secondary Treatment Tap Water Flush

    0

    500

    1000

    1500

    2000

    2500

    3000

    3500

    4000

    4500

    0.00 100.00 200.00 300.00 400.00 500.00 600.00

    time (hrs)

    biogas(ml)

    Anaerobic Secondary Treatment Deionized Water Flush Aerobic Secondary Treatment Tap Water Flush

    0

    500

    1000

    1500

    2000

    2500

    3000

    3500

    0.00 100.00 200.00 300.00 400.00 500.00 600.00

    t ime (hrs)

    biogas(ml)

    Anaerob ic Secondary Treatment De ionized Water Flush Aerob ic Secondary Treatment Tap Water F lush

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    Figure 22 Maximum vertical infiltration rate against landfill depth

    0.1

    1

    10

    100

    1000

    0 10 20 30 40 50 60

    Landfill depth (m)

    Max.Infiltrationrate(

    m/a)

    Variable KConstant K based on stress at base of landfillMinimum required flushing rate

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    Figure 23 Infiltration rate for a) K=2.1(')

    -2.71(best fit line on Fig. 15 for waste DM3); and

    b) K=17(')-3.26

    (worst case line on Fig. 15 for waste DM3) against landfill depth for various

    precompacted waste densities

    0.0001

    0.001

    0.01

    0.1

    1

    10

    0 10 20 30 40 50 60

    Landfill depth (m)

    Max.infiltrationrate(m/d)

    Min. flushing rate No pre-compaction 0.5 Mg/m3 0.75 Mg/m3

    0.9 Mg/m3 1.0 Mg/m3 1.1 Mg/m3 1.2 Mg/m3

    0.0001

    0.001

    0.01

    0.1

    1

    10

    0 10 20 30 40 50 60

    Landfill depth (m)

    Max.infiltrationrate(m/d)

    Min. flushing rate No pre-compaction 0.5 Mg/m3 0.75 Mg/m3

    0.9 Mg/m3 1.0 Mg/m3 1.1 Mg/m3 1.2 Mg/m3

    a)

    b)

    All waste densities at a water content (WCdry) of 51.5% (assumed WC of waste as deposited)

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    Figure 24 Relationship between discharge rate and drawdown for approximate ideal (a) confined and (b)

    unconfined aquifer analyses in which the hydraulic conductivity varies with drawdown according

    to K=2.1(')-2.71

    (best fit line on Fig. 15 for waste DM3).

    0.0E+00

    5.0E-05

    1.0E-04

    1.5E-04

    2.0E-04

    2.5E-04

    3.0E-04

    3.5E-04

    0 2 4 6 8 10

    Drawdown (m)

    Flowrate(m3/s)

    Variable K Constant K ( 4.09x10-6 m/s)

    a)

    0.0E+00

    1.0E-04

    2.0E-04

    3.0E-04

    4.0E-04

    5.0E-04

    6.0E-04

    7.0E-04

    0 5 10 15 20

    Drawdown (m)

    Flowrate(m3/s)

    Variable K Constant K (4.09x10-6 m/s)

    b)

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    Figure 25 Head distribution for injection wells and abstraction wells on parallel grid, with hydraulic

    conductivity based on unsaturated stress distribution.

    Figure 26 Variation of well discharge / injection rate with depth

    10

    12

    14

    16

    18

    20

    22

    24

    26

    28

    30

    0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6

    Flow rate per linear metre of well (m3/day)

    Depth(m)

    Pumped / Injection well: Kh=KvPumped / Injection well: Kh=2-5Kv

    Average pumped/ injection

    rate = 4.3 m3/day per well

    Average pumped/ injection rate

    = 68.1 m3/day per well

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    Table 1. Size and category analysis of waste AG2

    Size mm Weight

    %

    Pa/Cd PF Dp Tx Mc Mnc Gl Fe nFe Soil

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    Table 5. Size and category analysis of waste AG1

    Size mm Weight % Pa/Cd PF Dp Tx Mc Mnc Gl Put Fe nFe

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    Table 8 Variation in particle density, particle compressibility and waste compressibility with applied stress

    Average stress at end of stage, kPa 34 65 120 241 463

    Average particle density, t/m3 0.88 0.97 1.02 1.17 1.30

    Average particle compressibility, MPa-1

    - 5.38* 1.62 1.85 0.81

    Overall compressibility of waste, MPa-1 7.45 3.75 3.76 2.30 1.07

    a) Raw household waste DM3

    Average stress at end of stage, kPa 35 68 127 253 486

    Average particle density, t/m3 0.59 0.68 0.72 0.78 0.93

    Average particle compressibility, MPa-1

    - 6.60* 1.65 1.11 1.22*

    Overall compressibility of waste, MPa-1 7.29 6.18 4.12 1.45 0.87

    b) Pulverized household waste PV1

    Average stress at end of stage, kPa 35 67 123 239 458

    Average particle density, t/m3

    1.64 1.62 1.64 1.69 1.86

    Average particle compressibility, MPa-1 - -0.67* 0.36 0.49 0.73*

    Overall compressibility of waste, MPa-1

    7.38 3.85 2.91 1.57 0.66

    c) Aged household waste AG1

    * It is not possible for the average compressibility of the particles to be greater than the overall compressibility of

    the waste, and unlikely that it is negative. These values must therefore be in error to some extent.

    Table 9 Summary of total solids and total volatile solids destroyed in 30 litre SBAFB (Static Bed

    Anaerobic Flushing Bioreactor) system.

    Substrate: 60 : 40 mixed paper : food waste BMP: 0.546 m3

    CH4

    / Kg TS destroyed

    Reactor mode of operation % TS destroyed % TVS destroyed

    HRT 24 hrs - untreated leachate 6.49 3.92

    HRT 24 hrs - clean tap water 43.92 42.58

    HRT 48 hrs - clean tap water 41.68 40.55

    HRT 96 hrs - clean tap water 45.59 47.43

    HRT - hydraulic retention time BMP - biological methane potential

    TS - total solids TVS - total volatile solids

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    APPENDIX A

    References

    ASTM D 5298-92 Standard test method for measurement of soil potential (suction) using filter paper

    Committee D-18 on soil and rock. Approved September 15 1992, Published November 1992, Designated as D5298-92

    DoE (1994)National Household Waste Analysis Project - Phase 2 Volume 1 Report on composition and weight

    data Report No CWM 082/94 produced for the Waste Technical Division of the Department of the Environment

    under Research Contract PECD 7/10/288 by Warren Spring Laboratory and Aspinwall & Co.

    DoE (1995)Landfill design construction and operational practice Waste Management Paper 26B. HMSO,

    London 289pp

    Knox, K. (1990) The relationship between leachate and gas Proc. of the International conference on Landfill

    Gas: Energy and Environment. ISBN 0-7058-1628-1.

    Knox, K. (1996)A review of the Brogborough and Landfill 2000 test cells monitoring data. Final report for the

    Environment Agency R&D Technical Report P231. 113pp.

    Wingfield-Hayes, C., Fleming, G. and Gronow, J. (1997) Field trials of waste manipulation techniques: the

    Mid-Auchencarroch experimental landfill Proc. 6th International Sardinia Landfill Symposium. S. Margherita di

    Pula, Cagliari, Italy. Vol I pp 311-322. October 1997

    APPENDIX B

    Publications arising directly from this research

    Beaven, R.P. (1997). Hydraulic and Engineering Properties of Household Waste Proceedings of the IBC

    conference on "Designing and Managing Sustainable Landfill". 26-27 February. Scientific Societies Lecture

    Theatre. London

    Beaven, R.P. (1997). Is accelerated s tabilisation achievable? Paper presented at the IWM 1997 annual

    conference - Torbay 10 June.

    Beaven, R.P. (2000). The hydrogeological and geotechnical properties of household waste in relation to

    sustainable landfilling PhD Dissertation, University of London.

    Beaven, R.P. and Powrie, W. (1996). Determination of the Hydrogeological and Geotechnical Properties ofRefuse in relation to Sustainable Landfilling. Paper presented at the Nineteenth International Madison Waste

    Conference, September 25-26, 1996, Department of Engineering Professional Development, University of

    Wisconsin-Madison. USA.

    Beaven, R.P. and Powrie, W. (1999)Analysis of waste flushing and flow to wells using MODFLOW and an

    effective stress dependent hydraulic conductivity Proceedings Sardinia 99, Seventh International Waste

    Management and Landfill Symposium, S. Margherita di Pula, Cagliari, Italy; 4-8 October 1999. Vol II pp 33-41.

    Hudson, A.P., Beaven, R.P. and Powrie, W. (1999)Measurement of the hydraulic conductivity of household

    waste in a large scale compression cell Proceedings Sardinia 99, Seventh International Waste Management

    and Landfill Symposium, S. Margherita di Pula, Cagliari, Italy; 4-8 October 1999. Vol III pp 461-468.

    IWM (1999) The role and operation of the flushing bioreactorReport of the Institute of Wastes Management

    Sustainable Landfill Working Group. Pub. IWM Business Services Ltd.

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    Knox, K. (1996)A review of the Brogborough and Landfill 2000 test cells monitoring data. Final report for the

    Environment Agency Technical Report P231

    Parker, L.P., White, J.K. and Powrie, W (1999) The measurement of the geotechnical and hydrogeological

    properties of degrading solid waste Proceedings Sardinia 99, Seventh International Waste Management and

    Landfill Symposium, S. Margherita di Pula, Cagliari, Italy; 4-8 October 1999. Vol III pp 469-478.

    Powrie, W. and Beaven, R.P. (1998) Hydraulic conductivity of waste - current research and implications for

    leachate management Waste Management November 1998 pp22-23.

    Powrie, W. and Beaven, R.P. (1999) The hydraulic properties of household waste and implications for

    landfills Proceedings of the Institution of Civil Engineers, Geotechnical Engineering, Vol 137, Oct 1999, pp235-

    247.

    Powrie, W., Beaven, R.P. and Harkness. (1999).Applicabili ty of soil mechanics principles to household waste

    Proceedings Sardinia 99, Seventh International Waste Management and Landfill Symposium, S. Margherita di

    Pula, Cagliari, Italy; 4-8 October 1999. Vol III, pp429-436.

    Powrie, W., Richards, D. and Beaven, R.P. (1998). Compression of waste and implications for practice. Proc of

    the Symposium on Geotechnical Engineering of landfills. pp 3-18. Held at Nottingham Trent University 24

    September 1998 by the East Midlands Geotechnical Group of the ICE. Ed. Dixon, N. et al; Pub. Thomas Telford

    Ltd. ISBN 0 7277 2708 7.

    Walker, A.N., Beaven, R.P. and Powrie, W. (1997). Overcoming problems in the development of a high rate

    flushing bioreactor Proc. 6th International Sardinia Landfill Symposium. S. Margherita di Pula, Cagliari, Italy.

    Vol I pp 397-408. October 1997.

    Walker, A.N., Beaven, R.P. and Powrie, W. (1998). A conceptual design for sustainable landfill Proceedings of

    the 18th annual IAH groundwater seminar, Portlaoise, Ireland; April 1998. pp1-13.


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