Delta-Wye (Δ-Y) Transformation Calculator

Convert a three-terminal resistor network between Delta (Δ/Pi) and Wye (Y/Star) form.
Delta → Wye
Wye → Delta

Delta (Δ) to Wye (Y)

Ra=RabRca/Σ   Rb=RabRbc/Σ   Rc=RbcRca/Σ   where Σ=Rab+Rbc+Rca
Balanced 100Ω each
10/20/30Ω
Motor winding 30Ω each
Enter values and press Calculate.

Wye (Y) to Delta (Δ)

Rabp/Rc   Rbcp/Ra   Rcap/Rb   where Σp=RaRb+RbRc+RcRa
Balanced 33.3Ω each
5/10/15Ω
Star winding 10Ω each
Enter values and press Calculate.

Delta-Wye Transformation Explained

A three-terminal resistor network can be wired either as a Delta (Δ, also called Pi or mesh — three resistors forming a triangle between terminals A, B, C) or a Wye (Y, also called Star or Tee — three resistors meeting at a common center node, one running to each terminal). The two forms are electrically equivalent at the three terminals if their resistances follow the transformation formulas below, which lets you simplify bridge circuits, ladder networks, and three-phase loads that are not simple series/parallel combinations.

DirectionFormula
Δ→Y: RaRabRca/(Rab+Rbc+Rca)
Δ→Y: RbRabRbc/(Rab+Rbc+Rca)
Δ→Y: RcRbcRca/(Rab+Rbc+Rca)
Y→Δ: Rab(RaRb+RbRc+RcRa)/Rc
Y→Δ: Rbc(RaRb+RbRc+RcRa)/Ra
Y→Δ: Rca(RaRb+RbRc+RcRa)/Rb
Balanced (all equal) caseRY = RΔ/3  or  RΔ = 3×RY

This exact 3× relationship only holds when the three resistors are equal (the balanced/symmetric case, as with a balanced three-phase load); for unequal resistors the full formulas above must be used.

Real-World Applications & Examples

Worked examples

1. Balanced delta, 100 Ω each. Σ=300Ω → Ra=Rb=Rc=100×100/300=33.3 Ω each (confirms RY=RΔ/3).
2. Unequal delta. Rab=10, Rbc=20, Rca=30 Ω: Σ=60 → Ra=10×30/60=5 Ω, Rb=10×20/60=3.33 Ω, Rc=20×30/60=10 Ω.
3. Three-phase delta motor winding. Each phase winding 30 Ω in delta converts to an equivalent star winding of 30/3=10 Ω per phase for per-phase analysis.
4. Balanced wye back to delta. Ra=Rb=Rc=33.3Ω: Σp=3×33.3²≈3327 → Rab=Rbc=Rca=3327/33.3≈100 Ω — recovers the original delta exactly.
5. Unbalanced Wheatstone bridge. Converting one triangle of the bridge (say the R1-R2-Rg loop) to a star turns the bridge into a simple series-parallel network that can be solved directly for the galvanometer branch current.
6. Unequal wye, 5/10/15 Ω. Σp=5×10+10×15+15×5=50+150+75=275 → Rab=275/15=18.3 Ω, Rbc=275/5=55 Ω, Rca=275/10=27.5 Ω.

Frequently Asked Questions

What is a Delta-Wye (star-delta) transformation?

A mathematical technique that converts a three-terminal resistor network from a triangular Delta (Δ) arrangement to an equivalent center-tapped Wye (Y) arrangement, or vice versa, so that the network behaves identically at the three external terminals.

When do I need this transformation?

When a resistive network (like an unbalanced Wheatstone bridge or a three-phase load) cannot be reduced using simple series/parallel rules alone. Converting one triangle to a star (or vice versa) exposes series/parallel paths.

What is the shortcut for a balanced (equal-resistor) network?

If all three delta resistors are equal (RΔ), the equivalent wye resistors are each RΔ/3. Conversely, an equal-resistor wye (RY) converts to a delta of 3×RY per resistor.

Does the transformation change the power dissipated?

No — the equivalence is only valid as seen from the three terminals for terminal voltages/currents; internal dissipation in the converted network can differ, so do not use it to analyze internal losses of the original network directly.

Why is it also called Pi-Tee or star-mesh transformation?

In filter/RF design the delta topology is called Pi (Π) and the wye is called Tee (T); "star-mesh" is another name for the same wye/delta pair used in network theory.

Is the Delta-Y transform reversible?

Yes, it is fully reversible — converting Delta→Wye and then Wye→Delta with the correct formulas returns the original resistor values exactly.

How is this used in three-phase power systems?

Loads and transformer windings can be connected in either delta or star (wye); the transformation lets you convert per-phase impedances between the two connection types for load and fault analysis.

Can this be used for impedances (AC circuits), not just resistors?

Yes, the same formulas apply directly to complex impedances Zab, Zbc, Zca and Za, Zb, Zc in AC analysis.

What is the physical meaning of the wye center node?

It is a new, non-physical internal node created purely by the mathematical transformation; it does not exist in the original delta network and has no direct external connection.

How does this help solve a Wheatstone bridge that is not balanced?

Converting the delta formed by three of the bridge's resistors into a wye eliminates the bridging branch, turning the circuit into an ordinary series-parallel network solvable with basic rules.

What happens if one delta resistor is much larger than the others?

The corresponding wye resistors that share it in the numerator become relatively large too, while the wye resistor not touching that large resistor tends to be small — the transform still holds exactly, just with widely different magnitudes.

Is there a risk of getting the terminal labeling wrong?

Yes — consistently label terminals A, B, C on both networks. Ra is always the wye arm to terminal A, and it always pairs with the two delta resistors Rab and Rca that also touch terminal A.

Does this transformation work for more than three terminals?

The classic delta-wye/star-mesh transform is specifically for three-terminal networks; general star-mesh transforms exist for more terminals but use a different (more complex) formula set.

Can I use this for PCB trace resistance networks?

Yes — triangular ground or power-plane resistance meshes can be reduced to a star for quick IR-drop estimates at each of the three connection points.

Why does the sum term differ between the two directions?

Delta→Wye divides by the sum of the three delta resistors (Σ=Rab+Rbc+Rca); Wye→Delta divides by one wye resistor at a time using the sum of pairwise products (Σp=RaRb+RbRc+RcRa) — they are inverse operations, not mirror formulas.

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