الشرائح

Wye-Delta Transformations

12 دقيقة قراءة

Mansoura University
Mansoura University
Faculty of Computers and Information
Department of Information Technology
First Semester
Faculty of Computers and Information
Intro to Physics · Lesson 4
Wye-Delta Transformations
Prepared by Muhammad Elsayed
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ملاحظات الدرس

Wye-Delta Transformations

When series and parallel run out

Series and parallel reduction solves most networks, but not all of them.

  • In a bridge circuit no two resistors share exactly one node with nothing else attached, so neither rule applies.
  • The fix is to swap one three-terminal shape for its equivalent: a Y (also drawn as a tee) becomes a Δ (also drawn as a pi), or the other way round.
  • The swap is an equivalence, not an approximation: the resistance seen at every pair of terminals is identical before and after.

The two conversions

Both formulas come from setting the terminal-pair resistances equal, and both are easy to remember once you see the pattern.

  • Δ to Y: each wye resistor is the product of the two adjacent delta resistors divided by the sum of all three, so R1 = RbRc/(Ra+Rb+Rc).
  • Y to Δ: each delta resistor is the sum of the pairwise products divided by the opposite wye resistor, so Ra = (R1R2+R2R3+R3R1)/R1.
  • The balanced case is worth memorising: a delta of three equal R becomes a wye of R/3, and a wye of three equal R becomes a delta of 3R.

Working the problem

Transform once, then go back to the ordinary rules.

  • Pick the Δ or the Y that is blocking you, convert it, and the circuit usually falls apart into plain series and parallel steps.
  • Redraw after every step. Most mistakes in this topic are bookkeeping mistakes, not algebra.
  • DC Sweep in Multisim then confirms the answer by ramping the source and plotting the response instead of testing one value at a time.

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