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[[Category:ODE]]
[[Category:ODE]]
[[Category:time invariant]]
[[Category:time invariant]]
[[Category:parametric 1 parameter]]
[[Category:Parametric]]
[[Category:parametric 2-5 parameters]]
[[Category:affine parameter representation]]
[[Category:affine parameter representation]]
[[Category:first differential order]]
[[Category:first differential order]]
[[Category:SISO]]
{{Infobox
|Title          = Anemometer
|Benchmark ID    =
* anemometer1Param_n29008m1q1
* anemometer3Param_n29008m1q1
|Category        = misc
|System-Class    = AP-LTI-FOS
|nstates        = 29008
|ninputs        = 1
|noutputs        = 1
|nparameters    =
* 2
* 5
|components      = A, B, C, E
|License        = NA
|Creator        = [[User:Feng]]
|Editor          =
* [[User:Feng]]
* [[User:Himpe]]
* [[User:Lnor]]
* [[User:Baur]]
* [[User:Will]]
* [[User:Lund]]
|Zenodo-link    = NA
}}


==Description==
==Description==


An anemometer is a flow sensing device, consisting of a heater and
<figure id="fig:plot1">
temperature sensors before and after the heater, placed either
[[File:Model_Color.pdf|600px|thumb|right|<caption>Schematic 2D-Model-Anemometer</caption>]]
directly in the flow or in its vicinity. They are located on a membrane to
</figure>
minimize heat dissipation through the
<figure id="fig:plot2">
structure. Without any flow, the heat
 
dissipates symmetrically into the fluid. This symmetry is disturbed if
[[file:ContourPlot30.pdf|600px|thumb|right|<caption>Calculated temperature profile for the Anemometer function</caption>]]
a flow is applied to the fluid, which leads to a convection on the
 
temperature field and therefore to a difference between the
</figure>
temperature sensors (see Fig.1 below) from which the fluid
velocity can be determined.


The physical model can be expressed by the
An '''Anemometer'''<ref name="ernst01" group="a)"/><ref name="benner05" group="a)"/><ref name="moosmann05" group="a)"/><ref name="moosmann07" group="c)"/><ref name="moosmann05b" group="c)"/><ref name="rudnyi06" group="c)"/> (see [[wikipedia:Thermal_mass_flow_meter|thermal mass flow meter]])
convection-diffusion partial differential equation [4]:
is a flow sensing device, consisting of a heater and temperature sensors before and after the heater, placed either directly in the flow or in its vicinity Fig.&nbsp;1.
They are located on a membrane to minimize heat dissipation through the structure.
Without any flow, the heat dissipates symmetrically into the fluid.
This symmetry is disturbed if a flow is applied to the fluid,
which leads to a convection on the temperature field and therefore to a difference between the temperature sensors (see Fig.&nbsp;2) from which the fluid velocity can be determined.


<math>\rho c \frac{\partial T}{\partial t} = \nabla \cdot (\kappa
The physical model can be expressed by the [[wikipedia:Convection–diffusion_equation|convection-diffusion partial differential equation]] <ref name="moosmann04" group="b)"/>:
  \nabla T ) - \rho c v \nabla T + \dot q,</math>


where <math>\rho</math> denotes the mass density, <math>c</math> is the specific heat,
:<math>
<math>\kappa</math> is the thermal conductivity, <math>v</math> is the fluid
\rho c \frac{\partial T}{\partial t}
velocity, <math>T</math> is the temperature, and <math>\dot q</math> is the heat flow into the system
= \nabla \cdot (\kappa \nabla T)
caused by the heater.
- \rho c v \nabla T
+ \dot{q},
</math>


The solid model has been generated and meshed in ANSYS.
where <math>\rho</math> denotes the mass density, <math>c</math> is the specific heat capacity, <math>\kappa</math> is the thermal conductivity,
Triangular PLANE55 elements have been used for the finite element discretization. The order of the system is <math>n = 29008</math>.
<math>v</math> is the fluid velocity, <math>T</math> is the temperature, and <math>\dot q</math> is the heat flow into the system caused by the heater.


The solid model has been generated and meshed in [[wikipedia:ANSYS|ANSYS]].
Triangular [http://www.ansys.stuba.sk/html/elem_55/chapter4/ES4-55.htm PLANE55] elements have been used for the finite element discretization.
The order of the system is <math>n = 29008</math>.


Example with 1 parameter:
Example with one parameter:


The <math>n</math> dimensional ODE system has the following transfer function
The <math>n</math> dimensional [[wikipedia:Ordinary_Differential_Equation|ODE]] system has the following transfer function
<math>
:<math>
G(p) = C((sE - A1- p(A2 - A1))^{-1}B)
G(s, p) = C (s E - A_1 - p (A_2 - A_1))^{-1} B
</math>
</math>


with the fluid velocity <math>p(=v)</math> as single parameter.
with the fluid velocity <math>p(=v)</math> as single parameter.
Here <math>E</math> is the heat capacitance matrix, <math>B</math> is the load vector which is derived from separating the spatial and temporal variables in <math>\dot{q}</math> and the FEM discretization w.r.t. the spatial variables. <math>Ai</math> are the stiffness matrices with <math>i=1</math> for pure diffusion and <math>i=2</math> for diffusion and convection. Thus, for obtaining pure convection you have to compute <math>A2 - A1</math>.
Here <math>E</math> is the heat capacitance matrix, <math>B</math> is the load vector which is derived from separating the spatial and temporal variables in <math>\dot{q}</math> and the [[wikipedia:Finite_Element_Method|FEM]] discretization w.r.t. the spatial variables.
<math>A_i</math> are the stiffness matrices with <math>i=1</math> for pure diffusion and <math>i=2</math> for diffusion and convection.
Thus, for obtaining pure convection you have to compute <math>A_2 - A_1</math>.


Example with 3 parameters:
Example with three parameters:


Here, all fluid properties are identified as parameters. Thus, we consider the following transfer function
Here, all fluid properties are identified as parameters. Thus, we consider the following transfer function


<math>
:<math>
  G(p_0, p_1,p_2)     = C((s \underbrace{(E_s +   p_0 E_f)}_{E(p_0)}   - \underbrace{( A_{d,s} + p_1   A_{d,f} +   p_2 A_c )}_{A(p_1,p_2)} )^{-1}B)
G(s, p_0, p_1, p_2) =
C
(
  s \underbrace{(E_s + p_0 E_f)}_{E(p_0)}
  - \underbrace{(A_{d,s} + p_1 A_{d,f} + p_2 A_c)}_{A(p_1,p_2)}
)^{-1}
B
</math>
</math>


with parameters <math>p_0, \, p_1, \, p_2</math> which are combinations of the original fluid parameters <math>\rho, \, c, \, \kappa, \, v: \quad p_0 = \rho c, \, p_1=\kappa,</math> and <math>p_2 =\rho c v,</math> see [5]. So far, we have considered the mass density as fixed, i.e. <math>\rho=1</math>.
with parameters <math>p_0</math>, <math>p_1</math>, <math>p_2</math> which are combinations of the original fluid parameters <math>\rho</math>, <math>c</math>, <math>\kappa</math>, <math>v</math>: <math>p_0 = \rho c</math>, <math>p_1 = \kappa</math>, and <math>p_2 = \rho c v</math>, see <ref name="baur11" group="c)"/>. So far, we have considered the mass density as fixed, i.e. <math>\rho=1</math>.


==Origin==
==Origin==


IMTEK Freiburg, group of Jan Korvink.
* [http://www.imtek.uni-freiburg.de/professuren/simulation/  IMTEK Freiburg, Simulation group], Prof Dr Jan G. Korvink has taken on a position as Director of the Institute of Microstructure Technology (IMT) at the Karlsruhe Institute of Technology (KIT).


==Data==
==Data==


Matrices are in the Matrix Market format(http://math.nist.gov/MatrixMarket/). All matrices (for the one parameter system and for the three parameter case) can be found and uploaded in [[Media:Anemometer.tar.gz|Anemometer.tar.gz]]. The matrix name is used as an extension of the matrix file.  
Matrices are in the [http://math.nist.gov/MatrixMarket/ Matrix Market] format.
The system matrices have been extracted from ANSYS models by means of mor4fem.
All matrices (for the one parameter system and for the three parameter case) can be found and uploaded in [[Media:Anemometer.tar.gz|Anemometer.tar.gz]].
The matrix name is used as an extension of the matrix file.  
The system matrices have been extracted from ANSYS models by means of [http://simulation.uni-freiburg.de/downloads/mor4fem mor4fem].
For more information about computing the system matrices, the choice of the output, applying the permutation, please look into the [[media:Readme2.pdf|readme file]]. [[File: Readme2.pdf|thumb]]
For more information about computing the system matrices, the choice of the output, applying the permutation, please look into the [[media:Readme2.pdf|readme file]]. [[File: Readme2.pdf|thumb]]


To test the quality of the reduced order systems, harmonic simulations as well as transient step responses could be computed, see [5].
Example with one parameter:


* <tt>.B</tt>: load vector
* <tt>.E</tt>: heat capacitance matrix
* <tt>.P</tt>: permutation matrix
* <tt>.A</tt>: stiffness matrices (2)


Example with 1 parameter:
Example with three parameters:


*.B: load vector
* <tt>.B</tt>: load vector
*.E: damping matrix
* <tt>.E</tt>: heat capacitance matrices (2)
*.P: permutation matrix
* <tt>.A</tt>: stiffness matrices (5)
*.A: stiffness matrices (2)


Example with 3 parameters:
To test the quality of the reduced order systems, harmonic simulations as well as transient step responses could be computed, see <ref name="baur11" group="c)"/>.
 
The output matrix <math>C \in \mathbb{R}^{1 \times 29008}</math> is a vector with non-zero elements <math>C_{173} = 1</math> and <math>C_{133} = -1</math>.
 
==Dimensions==
 
System structure (1 parameter):
 
:<math>
\begin{align}
E \dot{x}(t) &= (A_1 + p (A_2 - A_1)) x(t) + B u(t) \\
y(t) &= Cx(t)
\end{align}
</math>
 
System dimensions:
 
<math>E \in \mathbb{R}^{29008 \times 29008}</math>,
<math>A_{1,2} \in \mathbb{R}^{29008 \times 29008}</math>,
<math>B \in \mathbb{R}^{29008 \times 1}</math>,
<math>C \in \mathbb{R}^{1 \times 29008}</math>.
 
 
System structure (3 parameter):
 
:<math>
\begin{align}
(E_1 + p_0 (E_2 - E_1)) \dot{x}(t) &= (A_1 + p_1 (A_3 - A_1 + A_4 - A_5) + p_2 (A_2 - A_1)) x(t) + B u(t) \\
y(t) &= Cx(t)
\end{align}
</math>
 
System dimensions:
 
<math>E_{1,2} \in \mathbb{R}^{29008 \times 29008}</math>,
<math>A_{1,2,3,4,5} \in \mathbb{R}^{29008 \times 29008}</math>,
<math>B \in \mathbb{R}^{29008 \times 1}</math>,
<math>C \in \mathbb{R}^{1 \times 29008}</math>.
 
==Citation==
 
To cite this benchmark, use the following references:
 
* For the benchmark itself and its data:
::The MORwiki Community, '''Anemometer'''. MORwiki - Model Order Reduction Wiki, 2018. http://modelreduction.org/index.php/Anemometer
 
@MISC{morwiki_anemom,
  author =      <nowiki>{{The MORwiki Community}}</nowiki>,
  title =        {Anemometer},
  howpublished = {{MORwiki} -- Model Order Reduction Wiki},
  url =          <nowiki>{https://modelreduction.org/morwiki/index.php/Anemometer}</nowiki>,
  year =        {2018}
}
 
* For the background on the benchmark:  


*.B: load vector
*.E: damping matrices (2)
*.A: stiffness matrices (5)


==References==
==References==


a) About the anemometer
a) About the '''Anemometer'''


<references group="a)">


[1] H. Ernst, "High-Resolution Thermal Measurements in Fluids," PhD thesis, University of Freiburg, Germany (2001).
<ref name="ernst01" group="a)">H. Ernst, "<span class="plainlinks">[http://www.freidok.uni-freiburg.de/volltexte/201/ High-Resolution Thermal Measurements in Fluids]</span>," PhD thesis, University of Freiburg, Germany (2001).</ref>


[2] P. Benner, V. Mehrmann and D. Sorensen, "Dimension Reduction of Large-Scale Systems," Lecture Notes in Computational Science and Engineering, Springer-Verlag, Berlin/Heidelberg, Germany, 45, 2005.
<ref name="benner05" group="a)">P. Benner, V. Mehrmann and D. Sorensen, "<span class="plainlinks">[http://dx.doi.org/10.1007/3-540-27909-1 Dimension Reduction of Large-Scale Systems]</span>", Lecture Notes in Computational Science and Engineering, Springer-Verlag, Berlin/Heidelberg, Germany, 45, 2005.</ref>
    
    
[3] C. Moosmann and A. Greiner, "Convective Thermal Flow Problems," Chapter 16 (pages 341--343) of [2].
<ref name="moosmann05" group="a)">C. Moosmann and A. Greiner, "<span class="plainlinks">[http://dx.doi.org/10.1007/3-540-27909-1_16 Convective Thermal Flow Problems]</span>", Chapter 16 (pages 341--343) of 2.</ref>


</references>


b) MOR for non-parametrized anemometer


b) MOR for non-parametrized '''Anemometer'''


[4] C. Moosmann, E. B. Rudnyi, A. Greiner and J. G. Korvink, "Model Order Reduction for Linear Convective Thermal Flow,"
<references group="b)">
Proceedings of 10th International Workshops on THERMal INvestigations of ICs and Systems, THERMINIC2004, 29 Sept - 1 Oct, 2004, Sophia Antipolis, France.


<ref name="moosmann04" group="b)">C. Moosmann, E. B. Rudnyi, A. Greiner and J. G. Korvink, "<span class="plainlinks">[http://modelreduction.com/doc/papers/moosmann04THERMINIC.pdf Model Order Reduction for Linear Convective Thermal Flow]</span>",
Proceedings of 10th International Workshops on THERMal INvestigations of ICs and Systems, THERMINIC2004, 29 Sept - 1 Oct, 2004, Sophia Antipolis, France.</ref>


c) MOR for parametrized anemometer
</references>




[5] U. Baur, P. Benner, A. Greiner, J. G. Korvink, J. Lienemann and C. Moosmann, "Parameter preserving model order reduction for MEMS applications," MCMDS Mathematical and Computer Modeling of Dynamical Systems, 17(4):297--317, 2011.
c) MOR for parametrized '''Anemometer'''


[6] C. Moosmann, "ParaMOR - Model Order Reduction for parameterized MEMS applications," PhD thesis, University of Freiburg, Germany (2007).
<references group="c)">


[7] C. Moosmann, E. B. Rudnyi, A. Greiner, J. G. Korvink and M. Hornung, "Model Order Reduction of a Flow Meter," Technical Proceedings of the 2005 Nanotechnology
<ref name="baur11" group="c)">U. Baur, P. Benner, A. Greiner, J. G. Korvink, J. Lienemann and C. Moosmann, "<span class="plainlinks">[http://dx.doi.org/10.1080/13873954.2011.547658 Parameter preserving model order reduction for MEMS applications]</span>", MCMDS Mathematical and Computer Modeling of Dynamical Systems, 17(4):297--317, 2011.</ref>
Conference and Trade Show, Nanotech 2005, May 8-12, 2005, Anaheim, California, USA, NSTINanotech
2005, vol. 3, p. 684-687.


[8] E. B. Rudnyi, C. Moosmann, A. Greiner, T. Bechtold, J. G. Korvink, "Parameter Preserving
<ref name="moosmann07" group="c)">C. Moosmann, "<span class="plainlinks">[http://www.freidok.uni-freiburg.de/volltexte/3971/ ParaMOR - Model Order Reduction for parameterized MEMS applications]</span>", PhD thesis, University of Freiburg, Germany (2007).</ref>
Model Reduction for MEMS System-level Simulation and Design," Proceedings of MATHMOD 2006, February 8 -
10, 2006, Vienna University of Technology, Austria.


<ref name="moosmann05b" group="c)">C. Moosmann, E. B. Rudnyi, A. Greiner, J. G. Korvink and M. Hornung, "<span class="plainlinks>[http://modelreduction.com/doc/papers/moosmann05MSM.pdf Parameter Preserving Model Order Reduction of a Flow Meter]</span>", Technical Proceedings of the 2005 Nanotechnology
Conference and Trade Show, Nanotech 2005, May 8-12, 2005, Anaheim, California, USA, NSTINanotech
2005, vol. 3, p. 684-687.</ref>


Fig. 1
<ref name="rudnyi06" group="c)">E. B. Rudnyi, C. Moosmann, A. Greiner, T. Bechtold, J. G. Korvink, "<span class="plainlinks">[http://modelreduction.com/doc/papers/rudnyi06mathmod.pdf Parameter Preserving Model Reduction for MEMS System-level Simulation and Design]</span>", Proceedings of MATHMOD 2006, February 8 -
 
10, 2006, Vienna University of Technology, Austria.</ref>
[[File:Model_Color.pdf|600px|thumb|left|Schemantic: 2D-model-anemometer]]


[[file:ContourPlot30.pdf|600px|thumb|left|Calculated temperature profile for anemometer function]]
</references>


==Contact==
==Contact==


[[User:Baur]]
[[User:Himpe]]

Latest revision as of 08:42, 11 June 2025


Anemometer
Background
Benchmark ID
  • anemometer1Param_n29008m1q1
  • anemometer3Param_n29008m1q1
Category

misc

System-Class

AP-LTI-FOS

Parameters
nstates
29008
ninputs

1

noutputs

1

nparameters
  • 2
  • 5
components

A, B, C, E

Copyright
License

NA

Creator

User:Feng

Editor
Location

NA


Description

Figure 1: Schematic 2D-Model-Anemometer
Figure 2: Calculated temperature profile for the Anemometer function

An Anemometer[a) 1][a) 2][a) 3][c) 1][c) 2][c) 3] (see thermal mass flow meter) is a flow sensing device, consisting of a heater and temperature sensors before and after the heater, placed either directly in the flow or in its vicinity Fig. 1. They are located on a membrane to minimize heat dissipation through the structure. Without any flow, the heat dissipates symmetrically into the fluid. This symmetry is disturbed if a flow is applied to the fluid, which leads to a convection on the temperature field and therefore to a difference between the temperature sensors (see Fig. 2) from which the fluid velocity can be determined.

The physical model can be expressed by the convection-diffusion partial differential equation [b) 1]:

ρcTt=(κT)ρcvT+q˙,

where ρ denotes the mass density, c is the specific heat capacity, κ is the thermal conductivity, v is the fluid velocity, T is the temperature, and q˙ is the heat flow into the system caused by the heater.

The solid model has been generated and meshed in ANSYS. Triangular PLANE55 elements have been used for the finite element discretization. The order of the system is n=29008.

Example with one parameter:

The n dimensional ODE system has the following transfer function

G(s,p)=C(sEA1p(A2A1))1B

with the fluid velocity p(=v) as single parameter. Here E is the heat capacitance matrix, B is the load vector which is derived from separating the spatial and temporal variables in q˙ and the FEM discretization w.r.t. the spatial variables. Ai are the stiffness matrices with i=1 for pure diffusion and i=2 for diffusion and convection. Thus, for obtaining pure convection you have to compute A2A1.

Example with three parameters:

Here, all fluid properties are identified as parameters. Thus, we consider the following transfer function

G(s,p0,p1,p2)=C(s(Es+p0Ef)E(p0)(Ad,s+p1Ad,f+p2Ac)A(p1,p2))1B

with parameters p0, p1, p2 which are combinations of the original fluid parameters ρ, c, κ, v: p0=ρc, p1=κ, and p2=ρcv, see [c) 4]. So far, we have considered the mass density as fixed, i.e. ρ=1.

Origin

  • IMTEK Freiburg, Simulation group, Prof Dr Jan G. Korvink has taken on a position as Director of the Institute of Microstructure Technology (IMT) at the Karlsruhe Institute of Technology (KIT).

Data

Matrices are in the Matrix Market format. All matrices (for the one parameter system and for the three parameter case) can be found and uploaded in Anemometer.tar.gz. The matrix name is used as an extension of the matrix file. The system matrices have been extracted from ANSYS models by means of mor4fem.

For more information about computing the system matrices, the choice of the output, applying the permutation, please look into the readme file.

Example with one parameter:

  • .B: load vector
  • .E: heat capacitance matrix
  • .P: permutation matrix
  • .A: stiffness matrices (2)

Example with three parameters:

  • .B: load vector
  • .E: heat capacitance matrices (2)
  • .A: stiffness matrices (5)

To test the quality of the reduced order systems, harmonic simulations as well as transient step responses could be computed, see [c) 4].

The output matrix C1×29008 is a vector with non-zero elements C173=1 and C133=1.

Dimensions

System structure (1 parameter):

Ex˙(t)=(A1+p(A2A1))x(t)+Bu(t)y(t)=Cx(t)

System dimensions:

E29008×29008, A1,229008×29008, B29008×1, C1×29008.


System structure (3 parameter):

(E1+p0(E2E1))x˙(t)=(A1+p1(A3A1+A4A5)+p2(A2A1))x(t)+Bu(t)y(t)=Cx(t)

System dimensions:

E1,229008×29008, A1,2,3,4,529008×29008, B29008×1, C1×29008.

Citation

To cite this benchmark, use the following references:

  • For the benchmark itself and its data:
The MORwiki Community, Anemometer. MORwiki - Model Order Reduction Wiki, 2018. http://modelreduction.org/index.php/Anemometer
@MISC{morwiki_anemom,
  author =       {{The MORwiki Community}},
  title =        {Anemometer},
  howpublished = {{MORwiki} -- Model Order Reduction Wiki},
  url =          {https://modelreduction.org/morwiki/index.php/Anemometer},
  year =         {2018}
}
  • For the background on the benchmark:


References

a) About the Anemometer

  1. H. Ernst, "High-Resolution Thermal Measurements in Fluids," PhD thesis, University of Freiburg, Germany (2001).
  2. P. Benner, V. Mehrmann and D. Sorensen, "Dimension Reduction of Large-Scale Systems", Lecture Notes in Computational Science and Engineering, Springer-Verlag, Berlin/Heidelberg, Germany, 45, 2005.
  3. C. Moosmann and A. Greiner, "Convective Thermal Flow Problems", Chapter 16 (pages 341--343) of 2.


b) MOR for non-parametrized Anemometer

  1. C. Moosmann, E. B. Rudnyi, A. Greiner and J. G. Korvink, "Model Order Reduction for Linear Convective Thermal Flow", Proceedings of 10th International Workshops on THERMal INvestigations of ICs and Systems, THERMINIC2004, 29 Sept - 1 Oct, 2004, Sophia Antipolis, France.


c) MOR for parametrized Anemometer

  1. C. Moosmann, "ParaMOR - Model Order Reduction for parameterized MEMS applications", PhD thesis, University of Freiburg, Germany (2007).
  2. C. Moosmann, E. B. Rudnyi, A. Greiner, J. G. Korvink and M. Hornung, "Parameter Preserving Model Order Reduction of a Flow Meter", Technical Proceedings of the 2005 Nanotechnology Conference and Trade Show, Nanotech 2005, May 8-12, 2005, Anaheim, California, USA, NSTINanotech 2005, vol. 3, p. 684-687.
  3. E. B. Rudnyi, C. Moosmann, A. Greiner, T. Bechtold, J. G. Korvink, "Parameter Preserving Model Reduction for MEMS System-level Simulation and Design", Proceedings of MATHMOD 2006, February 8 - 10, 2006, Vienna University of Technology, Austria.
  4. 4.0 4.1 U. Baur, P. Benner, A. Greiner, J. G. Korvink, J. Lienemann and C. Moosmann, "Parameter preserving model order reduction for MEMS applications", MCMDS Mathematical and Computer Modeling of Dynamical Systems, 17(4):297--317, 2011.

Contact

User:Himpe