simbuild 2012
TRANSCRIPT
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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
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
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
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
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
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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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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ApproachTemperature Data
Zoning Approximations
Koopman Modes
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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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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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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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Comparison of Koopman Modes
Koopman modes
illustrate thermalbehavior of zones
at different time
scales
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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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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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Comparison of Zoning Approximations
N
191 Zones
112 Zones
60 Zones
Floor 3 Floor 2 Floor 1
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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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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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Thank You
Questions?
This work was partially funded by Army Research OfficeGrant W911NF11-1-0511, with program manager Dr.
Sam StantonCollaborators:Erika EskenaziValerie EacretKazimir Gasljevic
Amorette Getty