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    Mezi Research Group

    Mezi Research Group

    Creating zoning approximationsto building energy models using

    the Koopman operatorMichael Georgescu

    Bryan EisenhowerIgor Mezi

    Department of Mechanical EngineeringUniversity of California, Santa Barbara

    SimBuild 2012Madison, WI

    August 1st, 2012

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    Mezi Research Group

    Mezi Research Group

    Introduction

    When creating building energy models, approximations are

    made to manage model complexity.

    One approximation is zoning, i.e., how the volume of a

    building is divided into regions where properties areassumed to be uniform.

    In practice, creating zoning approximations is performed

    cut-and-try.

    A systematic approach to zoning is introduced and used to

    study how model accuracy is influenced by a coarser

    building representation.

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    Mezi Research Group

    Mezi Research Group

    Modal Decompositions

    Structures

    http://www.lusas.com/case/bridge/images/bosphorus_mode_shapes.jpghttp://www.acs.psu.edu/drussell/Demos/2-dof-coupled/2-dof.html

    Spring Mass System

    In oscillatory systems, motion can be

    decomposed into normal modes.

    These modes depend on the structure,

    materials, and boundary conditions andexpress the motion of a system in terms

    of their characteristic behavior.

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    Courtesy of Jiazeng Shan

    http://www.lusas.com/case/bridge/images/bosphorus_mode_shapes.jpghttp://www.acs.psu.edu/drussell/Demos/2-dof-coupled/2-dof.htmlhttp://www.acs.psu.edu/drussell/Demos/2-dof-coupled/2-dof.htmlhttp://www.lusas.com/case/bridge/images/bosphorus_mode_shapes.jpg
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    Mezi Research Group

    Mezi Research Group

    Introduction (cont.)

    Temperature output from a building simulation can also be

    decomposed into modes.

    With a modal decomposition, influential features a building

    temperature evolution can be identified.

    Zoning approximations are created by calculating modes

    produced by a building simulation, and determining

    approximations based off of similarities in these modes.

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    Mezi Research Group

    Mezi Research Group

    The Koopman Operator

    )(1 jj xfx =+

    )())(()( 1+== jjj xgxfgxUg

    Given a finite dimensional nonlinear system

    (i.e. a building simulation)

    with output

    The Koopman operator, U, is defined as:

    Spectral properties of the Koopman operator are used to study the evolution of

    observables produced by building simulations

    [Mezi 2005, Nonlinear Dynamics]

    MMf :where

    Mg:

    The infinite dimensional, linear operator captures nonlinear, finite-

    dimensional dynamics

    Because the operator is unitary on the attractor, it can be studied through aspectral decomposition

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    Mezi Research Group

    Mezi Research Group

    Koopman Modes

    [Mezi 2005, Nonlinear Dynamics]

    Because the operator is unitary, the eigenvalue equation

    holdskkkU =

    Koopman modes describe the dynamics of observables at different frequencies,

    and will be the basis for model order reduction of building models

    is assumed to be in the span of eigenfunctions)(xg

    From this expression for , are a set of vectors called Koopman

    modes, and are coefficients of the projections of observables onto the

    eigenfunctions of the Koopman operator.

    =1}{ kkv)(xg

    =

    =

    1

    )()(

    k

    kkk vxxg Observables can be expressed in terms of

    eigenfunctions, , and

    eigenvalues , , of the operator

    k

    Mk :

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    Mezi Research GroupMezi Research Group

    Koopman Modes (cont.)

    [Mezi 2005, Nonlinear Dynamics]

    Koopman modes are calculated by taking harmonic averages of observables

    over the spatial field

    is in the span of eigenfunctions if is on the attractor)(xg 0x

    )())((

    1

    lim

    ))((1

    lim)(

    *21

    0

    )1(22

    1

    0

    2*

    xgexfgene

    xfgen

    xUg

    in

    j

    j

    ji

    n

    i

    n

    j

    j

    ji

    n

    =

    +

    =

    ==

    =

    )5.0,5.0[jie 2

    *g is a harmonic average

    are eigenvalues

    =

    =1

    0

    2* )(1

    lim)(n

    j

    j

    ji

    nxge

    nxg Note that

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    Mezi Research GroupMezi Research Group

    ApproachTemperature Data

    Zoning Approximations

    Koopman Modes

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    Mezi Research GroupMezi Research Group

    Name:Location:

    Size:Function:

    Floors:HVAC:

    Engineering Science Building

    Santa Barbara80,500 Square FeetUniversity Administration and Multi-functional Spaces3Combined mechanical and

    natural ventilation

    Building model created of the Engineering Science Building Model parameters determined from design drawings and

    measurement

    Zoning Case Study

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    Mezi Research GroupMezi Research Group

    Detailed Model Floorplan

    # ofZones

    Area(sqft)

    Total Building 191 80,500

    Offices 94 15,000

    Clean Room 14 10,000

    Laboratories 49 21,000

    Simulated Surfaces 2247

    Simulated Windows 478

    Floor 3

    Floor 1

    Floor 29/16

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    Mezi Research GroupMezi Research Group

    Koopman Operator Spectrum

    Koopman modes arecalculated based off

    of zone temperature Reduced zoning

    determined from

    modes which are

    largest in magnitude

    Period Max

    Min

    Mean

    8760 Hrs 3.459 1.000 2.040

    24 Hrs 2.055 0.121 0.626

    12 Hrs 0.788 0.022 0.136

    8 Hrs 0.371 0.004 0.048

    6 Hrs 0.221 0.006 0.029

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    Mezi Research GroupMezi Research Group

    Comparison of Koopman Modes

    Koopman modes

    illustrate thermalbehavior of zones

    at different time

    scales

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    Mezi Research GroupMezi Research Group

    Zoning approximations are created by merging adjacentzones similar KM magnitude and phase

    and are adjacent zones

    If zone and zone are within a pre-specified interval

    r, the zones are merged as one effective zone Shared walls of previously unmerged zones become

    internal masses to the new zone (if desired) By adjusting the value ofr, models with a desired

    amount of zone coarseness can be created

    Creating Zoning Approximations

    rxx jk

    ik

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    Mezi Research GroupMezi Research Group

    Detailed Model Floorplan

    # ofZones

    Area(sqft)

    Total Building 191 80,500

    Offices 94 15,000

    Clean Room 14 10,000

    Laboratories 49 21,000

    Simulated Surfaces 2247

    Simulated Windows 478

    Floor 3

    Floor 1

    Floor 213/16

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    Mezi Research GroupMezi Research Group

    Comparison of Zoning Approximations

    N

    191 Zones

    112 Zones

    60 Zones

    Floor 3 Floor 2 Floor 1

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    Mezi Research GroupMezi Research Group

    Results of Simplified Models

    Each model was simulated with a continuously operatingHVAC system (EnergyPlus Ideal Loads HVAC)

    Error is percentage difference in predicted HVAC energy

    HVAC Prediction Error

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    Mezi Research GroupMezi Research Group

    Summary

    Using properties of the Koopman operator, a systematicapproach to creating zoning approximations is shown

    A 191 zone model was reduced to 60 zones before a

    sharp increase occurs in the rate of prediction error

    With this method, neglecting the internal mass of

    unmodeled walls causes error to increase linearly

    Future work is to understand what causes fast growth of

    prediction error with coarser zoning

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    M i R h G

    M i R h G

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    Mezi Research GroupMezi Research Group

    Thank You

    Questions?

    [email protected]

    This work was partially funded by Army Research OfficeGrant W911NF11-1-0511, with program manager Dr.

    Sam StantonCollaborators:Erika EskenaziValerie EacretKazimir Gasljevic

    Amorette Getty