Star to delta Transformation And Vice Versa

 The Y-Δ transform, also written Y-delta, Wye-delta, Kennelly’s delta-star transformation, star-mesh transformation, T-Π or T-pi transform, is a mathematical technique to simplify the analysis of an electrical network.


Equations for the transformation from Δ-load to Y-load 3-phase circuit

The general idea is to compute the impedance Ry at a terminal node of the Y circuit with impedances R', R'' to adjacent nodes in the Δ circuit by
R_y = \frac{R'R''}{\sum R_\Delta}
where RΔ are all impedances in the Δ circuit. This yields the specific formulae
R_1 = \frac{R_aR_b}{R_a + R_b + R_c},
R_2 = \frac{R_bR_c}{R_a + R_b + R_c},
R_3 = \frac{R_aR_c}{R_a + R_b + R_c}.

Equations for the transformation from Y-load to Δ-load 3-phase circuit

The general idea is to compute an impedance RΔ in the Δ circuit by
R_\Delta = \frac{R_P}{R_\mathrm{opposite}}
where RP = R1R2 + R2R3 + R3R1 is the sum of the products of all pairs of impedances in the Y circuit and Ropposite is the impedance of the node in the Y circuit which is opposite the edge with RΔ. The formula for the individual edges are thus
R_a = \frac{R_1R_2 + R_2R_3 + R_3R_1}{R_2}
R_b = \frac{R_1R_2 + R_2R_3 + R_3R_1}{R_3}
R_c = \frac{R_1R_2 + R_2R_3 + R_3R_1}{R_1}

Graph theory

In graph theory, the Y-Δ transform means replacing a Y subgraph of a graph with the equivalent Δ subgraph. The transform preserves the number of edges in a graph, but not the number of vertices or the number of cycles. Two graphs are said to be Y-Δ equivalent if one can be obtained from the other by a series of Y-Δ transforms in either direction. For example, the Petersen graph family is a Y-Δ equivalence class.

Demonstration

Δ-load to Y-load transformation equations

Δ and Y circuits with the labels that are used in this article.
To relate {Ra,Rb,Rc} from Δ to {R1,R2,R3} from Y, the impedance between two corresponding nodes is compared. The impedance in either configuration is determined as if one of the nodes is disconnected from the circuit.
The impedance between N1 and N2 with N3 disconnected in Δ:
\begin{align} 
R_\Delta(N_1, N_2) &= R_b \parallel (R_a+R_c) \\
&= \frac{1}{\frac{1}{R_b}+\frac{1}{R_a+R_c}}    \\
&= \frac{R_b(R_a+R_c)}{R_a+R_b+R_c}.
\end{align}
To simplify, let's call RT the sum of {Ra,Rb,Rc}.
RT = Ra + Rb + Rc
Thus,
 R_\Delta(N_1, N_2) = \frac{R_b(R_a+R_c)}{R_T}
The corresponding impedance between N1 and N2 in Y is simple:
RY(N1,N2) = R1 + R2
hence:
R_1+R_2 = \frac{R_b(R_a+R_c)}{R_T}   (1)
Repeating for R(N2,N3):
R_2+R_3 = \frac{R_c(R_a+R_b)}{R_T}   (2)
and for R(N1,N3):
R_1+R_3 = \frac{R_a(R_b+R_c)}{R_T}.   (3)
From here, the values of {R1,R2,R3} can be determined by linear combination (addition and/or subtraction).
For example, adding (1) and (3), then subtracting (2) yields
R_1+R_2+R_1+R_3-R_2-R_3 =
  \frac{R_b(R_a+R_c)}{R_T}
+ \frac{R_a(R_b+R_c)}{R_T}
- \frac{R_c(R_a+R_b)}{R_T}
2R_1 = \frac{2R_bR_a}{R_T}
thus,
R_1 = \frac{R_bR_a}{R_T}.
where RT = Ra + Rb + Rc
For completeness:
R_1 = \frac{R_bR_a}{R_T} (4)
R_2 = \frac{R_bR_c}{R_T} (5)
R_3 = \frac{R_aR_c}{R_T} (6)

[edit] Y-load to Δ-load transformation equations

Let
RT = Ra + Rb + Rc.
We can write the Δ to Y equations as
R_1 =  \frac{R_aR_b}{R_T}   (1)
R_2 =  \frac{R_bR_c}{R_T}   (2)
R_3 =  \frac{R_aR_c}{R_T}.   (3)
Multiplying the pairs of equations yields
R_1R_2 = \frac{R_aR_b^2R_c}{R_T^2}   (4)
R_1R_3 = \frac{R_a^2R_bR_c}{R_T^2}   (5)
R_2R_3 = \frac{R_aR_bR_c^2}{R_T^2}   (6)
and the sum of these equations is
R_1R_2 + R_1R_3 + R_2R_3 = \frac{R_aR_b^2R_c +
 R_a^2R_bR_c + R_aR_bR_c^2}{R_T^2}   (7)
Factor RaRbRc from the right side, leaving RT in the numerator, canceling with an RT in the denominator.
R_1R_2 + R_1R_3 + R_2R_3 = 
\frac{(R_aR_bR_c)(R_a+R_b+R_c)}{R_T^2}
R_1R_2 + R_1R_3 + R_2R_3 = 
\frac{R_aR_bR_c}{R_T} (8)
-Note the similarity between (8) and {(1),(2),(3)}
Divide (8) by (1)
\frac{R_1R_2 + R_1R_3 + R_2R_3}{R_1} = 
\frac{R_aR_bR_c}{R_T}\frac{R_T}{R_aR_b},
\frac{R_1R_2 + R_1R_3 + R_2R_3}{R_1} = R_c,
which is the equation for Rc. Dividing (8) by R2 or R3 gives the other equations.