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Load Flow Study
Fast Decoupled Load Flow(FDLF)
Presented by-
fs
Overview
๏ต Fast decoupled load flow
๏ต Why FDLF?
๏ต Flowchart
๏ต Program
๏ต Output
๏ต Conclusion
๏ต Reference
Fast decoupled load flow
๏ต Algorithm is based on Newton-Raphson method.
๏ต When transmission lines has a high X/R ratio, the newton Raphson could be
further simplified.
๏ต Consider the Newton-Raphson load flow equation:
๏ต โˆ†๐‘ƒ are less sensitive to โˆ†|๐‘‰| and more sensitive to โˆ†๐›ฟ.
๏ต โˆ†๐‘„ are less sensitive to โˆ†๐›ฟ and more sensitive to โˆ†|๐‘‰| .
๏ต So, N and J elements can be eliminated.
โˆ†๐‘ƒ
โˆ†๐‘„
=
๐ป ๐‘
๐ฝ ๐ฟ
โˆ†๐›ฟ
โˆ†|๐‘‰|
............(1)
cos๐›ฟ๐‘–๐‘˜ โ‰… 1, sin๐›ฟ๐‘–๐‘˜ โ‰…0
G๐‘–๐‘— sin๐›ฟ๐‘–๐‘˜<<B๐‘–๐‘˜, and Q๐‘–<<B๐‘–๐‘–|V๐‘–|2
With these assumptions H and L are square submatrices of dimension (n-
1) and (m-1) respectively are:
For i = k, H๐‘–๐‘–=L ๐‘–๐‘– โ‰ˆ
- B๐‘–๐‘–|V๐‘–|2
For iโ‰  ๐‘˜, H๐‘–๐‘˜=L ๐‘–๐‘˜ โ‰ˆ- |V๐‘–| |V ๐‘˜| B๐‘–๐‘˜
With further simplification,the matrix equation for the solution of load
flow by FDLF method are:
โˆ†๐‘ƒ/|๐‘‰| = ๐ตโ€ฒ โˆ†๐›ฟ โ€ฆโ€ฆโ€ฆ..(2)
โˆ†๐‘„/|๐‘‰| = ๐ตโ€ฒโ€ฒ โˆ†|๐‘‰| โ€ฆ โ€ฆ โ€ฆ . (3)
Where, Bโ€™ and Bโ€ are matrices of elements -B๐‘–๐‘˜(i=2,โ€ฆ..n and k=2,โ€ฆ.n)
and -B๐‘–๐‘˜(i=2,โ€ฆ..,m and k=2,โ€ฆ.,m).
Why FDLF?
๏ต For practical accuracies, only 2-5 iterations are required.
๏ต More reliable than NR method
๏ต Speed is 5 times that of NR method
๏ต Storage requirement is 60 percent of NR
๏ต Constant jacobian
๏ต Physically justifiable assumptions
FLOWCHART:
calculate โˆ†๐‘ท๐’Š๐’“ for i=(2,3,4 โ€ฆ . โ€ฆ โ€ฆ ๐ง)(๐๐• ๐š๐ง๐ ๐๐ ๐›๐ฎ๐ฌ๐ž๐ฌ)
solve for โˆ† ๐œน๐’Š ๐’‡๐’๐’“ ๐’Š = ๐Ÿ, ๐Ÿ‘ โ€ฆ โ€ฆ ๐’
calculate โˆ†๐‘ธ๐’Š ๐’“ for i=(2,3,4 โ€ฆ . โ€ฆ โ€ฆ ๐ฆ)(๐๐ ๐›๐ฎ๐ฌ๐ž๐ฌ)
Solve for โˆ†|Vi| for i=2,3 โ€ฆ . โ€ฆ . m.
PROGRAM-
fdlf.txt
OUTPUT-
Conclusion
๏ต Due to constant jacobian, defining functions are not sensitive to any humps.
๏ต It can be employed in optimization studies.
๏ต Used for obtaining information of both real and reactive power for multiple
load flow studies.
References
๏ต M. A.PAI , Computer Techniques in Power System Analysis.
๏ต D.P. Kothari, Modern Power System Analysis .
THANK YOU!!!

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Fast Decoupled Load Flow Study: An SEO-Optimized Title Under 40 Characters

  • 1. Load Flow Study Fast Decoupled Load Flow(FDLF) Presented by- fs
  • 2. Overview ๏ต Fast decoupled load flow ๏ต Why FDLF? ๏ต Flowchart ๏ต Program ๏ต Output ๏ต Conclusion ๏ต Reference
  • 3. Fast decoupled load flow ๏ต Algorithm is based on Newton-Raphson method. ๏ต When transmission lines has a high X/R ratio, the newton Raphson could be further simplified. ๏ต Consider the Newton-Raphson load flow equation: ๏ต โˆ†๐‘ƒ are less sensitive to โˆ†|๐‘‰| and more sensitive to โˆ†๐›ฟ. ๏ต โˆ†๐‘„ are less sensitive to โˆ†๐›ฟ and more sensitive to โˆ†|๐‘‰| . ๏ต So, N and J elements can be eliminated. โˆ†๐‘ƒ โˆ†๐‘„ = ๐ป ๐‘ ๐ฝ ๐ฟ โˆ†๐›ฟ โˆ†|๐‘‰| ............(1)
  • 4. cos๐›ฟ๐‘–๐‘˜ โ‰… 1, sin๐›ฟ๐‘–๐‘˜ โ‰…0 G๐‘–๐‘— sin๐›ฟ๐‘–๐‘˜<<B๐‘–๐‘˜, and Q๐‘–<<B๐‘–๐‘–|V๐‘–|2 With these assumptions H and L are square submatrices of dimension (n- 1) and (m-1) respectively are: For i = k, H๐‘–๐‘–=L ๐‘–๐‘– โ‰ˆ - B๐‘–๐‘–|V๐‘–|2 For iโ‰  ๐‘˜, H๐‘–๐‘˜=L ๐‘–๐‘˜ โ‰ˆ- |V๐‘–| |V ๐‘˜| B๐‘–๐‘˜ With further simplification,the matrix equation for the solution of load flow by FDLF method are: โˆ†๐‘ƒ/|๐‘‰| = ๐ตโ€ฒ โˆ†๐›ฟ โ€ฆโ€ฆโ€ฆ..(2) โˆ†๐‘„/|๐‘‰| = ๐ตโ€ฒโ€ฒ โˆ†|๐‘‰| โ€ฆ โ€ฆ โ€ฆ . (3) Where, Bโ€™ and Bโ€ are matrices of elements -B๐‘–๐‘˜(i=2,โ€ฆ..n and k=2,โ€ฆ.n) and -B๐‘–๐‘˜(i=2,โ€ฆ..,m and k=2,โ€ฆ.,m).
  • 5. Why FDLF? ๏ต For practical accuracies, only 2-5 iterations are required. ๏ต More reliable than NR method ๏ต Speed is 5 times that of NR method ๏ต Storage requirement is 60 percent of NR ๏ต Constant jacobian ๏ต Physically justifiable assumptions
  • 6. FLOWCHART: calculate โˆ†๐‘ท๐’Š๐’“ for i=(2,3,4 โ€ฆ . โ€ฆ โ€ฆ ๐ง)(๐๐• ๐š๐ง๐ ๐๐ ๐›๐ฎ๐ฌ๐ž๐ฌ) solve for โˆ† ๐œน๐’Š ๐’‡๐’๐’“ ๐’Š = ๐Ÿ, ๐Ÿ‘ โ€ฆ โ€ฆ ๐’ calculate โˆ†๐‘ธ๐’Š ๐’“ for i=(2,3,4 โ€ฆ . โ€ฆ โ€ฆ ๐ฆ)(๐๐ ๐›๐ฎ๐ฌ๐ž๐ฌ)
  • 7. Solve for โˆ†|Vi| for i=2,3 โ€ฆ . โ€ฆ . m.
  • 9. Conclusion ๏ต Due to constant jacobian, defining functions are not sensitive to any humps. ๏ต It can be employed in optimization studies. ๏ต Used for obtaining information of both real and reactive power for multiple load flow studies.
  • 10. References ๏ต M. A.PAI , Computer Techniques in Power System Analysis. ๏ต D.P. Kothari, Modern Power System Analysis .