Statistical Calibration of Dynamic Ampacity Model Vclav mdl, - - PowerPoint PPT Presentation

statistical calibration of dynamic ampacity model
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Statistical Calibration of Dynamic Ampacity Model Vclav mdl, - - PowerPoint PPT Presentation

Statistical Calibration of Dynamic Ampacity Model Vclav mdl, Jaroslav najdr Regional Innovation Centre for Electrical Engineering (RICE) University of West Bohemia Pilsen, Czech Republic Institute of Information Theory and Automation,


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Statistical Calibration of Dynamic Ampacity Model

Václav Šmídl, Jaroslav Šnajdr

Regional Innovation Centre for Electrical Engineering (RICE) University of West Bohemia Pilsen, Czech Republic Institute of Information Theory and Automation, Prague, Czech Republic,

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  • Outline

Motivation Dynamic Ampacity Mathematical model Problem definition Proposed model Validation: real data

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  • Ampacity = Ampere capacity of a conductor

Limited by:

  • 1. Conductor thermal limit
  • 2. Minimal clearance of the ground

Why it is important (VARLEY, J. 2009):

  • 1. Demands for power transmission are unstable due to renewable sources,
  • 2. Large safety margin on ampacity remains unused,
  • 3. Too conservative limits on ampacity may yields energy money loss or

stability problems.

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  • CIGRE model of ampacity

Model: PJ + Ps + Pc = mccc dTc dt + Pr + Pk + Pw where: PJ are Joule conductive losses, PJ = RkI2

ef [1 + b(Tc − 273)],

Ps is solar heating, Ps = ǫσS(T 4

c − T 4 amb)

Pr is radiative cooling Pc is convective cooling Pk is corona heating Pw is water cooling

Properties

◮ complex non-linear model, ◮ uncertain inputs – weather conditions: solar, wind, rain

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  • Experimental line

Data from a line equipped by meteostations are available from ČEPS.

Measurements (irregular sampling):

◮ solar radiation intensity, ◮ wind velocity and angle ◮ ambient and surface conductor temperature

7.3466 7.3466 7.3466 7.3466 7.3466 7.3466 7.3466 7.3466 x 10

5

−200 200 400 600 800 1000 1200 1400 Solar activity

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  • Deterministic approach

00:00 06:00 12:00 18:00 00:00 −20 20 40 60 80 time Conductor temperature [°C] Model Measurement Difference

  • 1. The goal is to reach temperatures under a certain limit,

◮ errors can be used as safety margin

  • 2. Errors are not constant, they are state dependent
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  • Statistical approach

Goals

  • 1. Estimate not only the temperature but also the error bound.
  • 2. Calibrate the error bound for reliability

Challenges

  • 1. quantify uncertainty of the inputs (how can we trust the sensors,

potentially predictions)

  • 2. transform the uncertainty through the non-linear model,
  • 3. design model of corrections (callibration)
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  • Proposed model
  • 1. uncertainty of the inputs

◮ we operate on one hour window. Uncertainty is modeled by mean and

variance of the values.

  • 2. transform the uncertainty through the non-linear model,

◮ using sigma point transform on deterministic samples from the

distribution of the inputs

  • 3. design model of corrections (callibration)

◮ we estimate unknown multiplier, γ, of computed correlation

cov(Tc) = γcov(Tc,model),

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  • Validation: real data

610 620 630 640 650 660 15 20 25 30 35 40 ritherm Tcalc Tcalc std+ Tcalc std− Tritherm std+ Tritherm std− ∆opt 610 620 630 640 650 660 10 15 20 25 30 35 40 45 50 55 T [�C] ritherm implicit Tcalc Tcalc std+ Tcalc std− Tritherm std+ Tritherm std−

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  • Quantile-Quantile plot

−4 −3 −2 −1 1 2 3 4 −2 −1.5 −1 −0.5 0.5 1 1.5 Standard Normal Quantiles Quantiles of Input Sample QQ Plot of Sample Data versus Standard Normal

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  • Conclusion
  • 1. Maximum current through a transmission line is restricted by thermal

limit,

  • 2. Temperature of the conductor depends on weather conditions, which

are uncertain,

  • 3. Statistical models calibration aims to provide reliable uncertainty

bound

  • 4. Future work:

4.1 design of model for predicted weather, 4.2 model local corrections,