A12 Three-Phase Circuits

Updated 4 Oct 2026

Introduction


Balanced Three-Phase Voltages


Balanced Wye-Wye Connection



Balanced Wye-Delta Connection




Balanced Delta-Wye Connection


Balanced Delta-Delta Connection


Introduction

🌐 Three-Phase Circuits — Overview

  • A three-phase system is a type of polyphase system, where AC sources operate at the same frequency but are 120° out of phase with each other.
  • It’s the most common and economical method to generate, transmit, and distribute electrical power.

🧠 Why Is It Important?

  1. Nearly all electric power is generated and distributed using three-phase systems.
  2. It can provide constant (non-pulsating) power to loads.
  3. For the same amount of power, the three-phase system is more economical than the single-phase

🧲 How It Works

  • A three-phase generator consists of:
    • A rotating magnet (rotor)
    • A stationary coil system (stator) with windings spaced 120° apart
  • As the rotor spins, it induces AC voltages in the coils, each 120° apart in phase but equal in magnitude.

Balanced Three-Phase Voltages

Source and Load Connections

  • Voltage sources can be connected in:
    • Wye (Y) configuration
    • Delta (Δ) configuration
  • Loads can also be connected in:
    • Wye (Y) configuration
    • Delta (Δ) configuration

This results in four possible source-load combinations:

  • Y-Y
  • Y-Δ
  • Δ-Y
  • Δ-Δ

Balanced Conditions

  • All phase voltages have the same magnitude: ∣Van∣=∣Vbn∣=∣Vcn∣|V_{an}| = |V_{bn}| = |V_{cn}|
  • The sum of phase voltages is zero: Van+Vbn+Vcn=0V_{an} + V_{bn} + V_{cn} = 0

Phase Sequence

  • Defines the order in which voltages reach their peaks.

➕ Positive Sequence (abc)

Van=Vp∠0°Vbn=Vp∠−120°Vcn=Vp∠+120°\begin{aligned} V_{an} &= V_p\angle0° \\ V_{bn} &= V_p\angle-120° \\ V_{cn} &= V_p\angle+120° \\ \end{aligned}

➖ Negative Sequence (acb)

Van=Vp∠0°Vcn=Vp∠−120°Vbn=Vp∠+120°\begin{aligned} V_{an} &= V_p\angle0° \\ V_{cn} &= V_p\angle-120° \\ V_{bn} &= V_p\angle+120° \\ \end{aligned}

วิธีดูง่าย ๆ ถ้าให้กราฟมา ว่าเป็น Sequence อะไร คือขวาสุดจะเป็น Van{V_{an}} เสมอ แล้วไล่ Clockwise!! ก็จะรู้ว่าเป็นอะไรเลย

Balanced Loads

Wye (Y) Load:

Z1=Z2=Z3=ZY\mathbf{Z}_1 = \mathbf{Z}_2 = \mathbf{Z}_3 = \mathbf{Z}_Y

where ZY\mathbf{Z}_Y is the load impedance per phase.

Delta (Δ) Load:

Z1=Z2=Z3=ZΔ\mathbf{Z}_1 = \mathbf{Z}_2 = \mathbf{Z}_3 = \mathbf{Z}_\Delta

where ZΔ\mathbf{Z}_\Delta is the load impedance per phase.

Conversion between Y and Δ:

ZΔ=3ZY\mathbf{Z}_\Delta=3\mathbf{Z}_Y ZY=13ZΔ\mathbf{Z}_Y=\frac{1}{3}\mathbf{Z}_\Delta

Balanced Wye-Wye (Y-Y) Connection

🧠 What It Is

  • A Balanced Y-Y system is when both the source and load are Wye (Y) connected and balanced.
  • This configuration is the most important because:

Any balanced three-phase system can be reduced to an equivalent Y-Y system.

⚙️ Key Terms

TermMeaning
ZsSource impedance (internal generator winding)
ZlZ_lLine impedance (wires between source and load)
ZLZ_LLoad impedance per phase
ZYZ_YTotal impedance per phase (ZY = Zs + Zl + ZL)
VpV_pPhase voltage (line-to-neutral voltage)
VLV_LLine voltage (line-to-line voltage)
Ia,Ib,Ic\mathbf{I}_a,\mathbf{I}_b,\mathbf{I}_cLine currents (equal to phase currents in Y-Y)
Van,Vbn,Vcn\mathbf{V}_{an},\mathbf{V}_{bn},\mathbf{V}_{cn}Phase voltages for phases a, b, and c
Vab,Vbc,Vca\mathbf{V}_{ab},\mathbf{V}_{bc},\mathbf{V}_{ca}Line voltages between lines a-b, b-c, c-a
VAN,VBN,VCN\mathbf{V}_{AN},\mathbf{V}_{BN},\mathbf{V}_{CN}Load voltage
Load current

In a Y-Y system:
Line current = Phase current

Relationship Between Voltages

Phase Voltage (line to neutral):

Assume positive sequence (abc):

Van=Vp∠0°Vbn=Vp∠−120°Vcn=Vp∠+120°\begin{aligned} \mathbf{V}_{an} &= V_p\angle0° \\ \mathbf{V}_{bn} &= V_p\angle-120° \\ \mathbf{V}_{cn} &= V_p\angle+120° \\ \end{aligned}
  • ตรงตัวเลยเนอะ Phase Voltage (คือแต่ละสายเทียบกับสาย Neutral)

Line Voltage (line to line):

From vector subtraction:

Vab=Van−Vbn=3⋅Vp∠30°Vbc=Vbn−Vcn=3⋅Vp∠−90°Vca=Vcn−Van=3⋅Vp∠150°\begin{aligned} \mathbf{V}_{ab} = \mathbf{V}_{an}-\mathbf{V}_{bn} &= \sqrt{3}\cdot V_p\angle30° \\ \mathbf{V}_{bc} = \mathbf{V}_{bn}-\mathbf{V}_{cn} &= \sqrt{3}\cdot V_p\angle-90° \\ \mathbf{V}_{ca} = \mathbf{V}_{cn}-\mathbf{V}_{an} &= \sqrt{3}\cdot V_p\angle150° \\ \end{aligned}
  • Magnitude ของทั้งสามก็จะเท่ากันแหละ เข้าใจเนอะ แต่เป็น 3\sqrt{3} เท่าของ VpV_p แล้วก็นำหน้าอยู่ 30∘30^\circ
  • เลยทำให้เรารู้ Relationship แรก
Vab=3⋅Van∠30°\Huge{\boxed{\mathbf{V}_{ab} = \sqrt{3}\cdot \mathbf{V}_{an}\angle30°}}

Line and Phase Current

Since the system is balanced:

Ia=VanZY\mathbf{I}_a = \frac{\mathbf{V}_{an}}{\mathbf{Z}_Y}
  • ซึ่งมันก็คือ Ohm’s Law ธรรมดาเนี่ยแหละ
  • ส่วน Ib,Ic\mathbf{I}_b,\mathbf{I}_c ก็ค่อย Extend answer จาก Ia\mathbf{I}_a ไป ทีละ 120∘120^\circ แบบปกติเลย
  • Sum ของ Line Currents ทั้ง 3 Phase ก็เป็น 0 (นึกภาพแล้วอ่อเลยย) → In=0I_n=0

Step-by-Step Analysis Procedure

  1. Draw the single-phase equivalent circuit (typically phase A).
  • This simplifies the system to one phase with voltage Van\mathbf{V}_{an} and impedance ZY\mathbf{Z}_Y.
  1. Solve for the line/phase current in that phase: Ia=VanZY\mathbf{I}_a = \frac{\mathbf{V}_{an}}{\mathbf{Z}_Y}
  2. Extend solution to other phases using 120° phase shifts: Ib=Ia∠−120∘Ic=Ia∠+120∘\mathbf{I}_b=\mathbf{I}_a\angle-120^\circ \quad \quad \mathbf{I}_c=\mathbf{I}_a\angle+120^\circ
  3. Use vector relationships to find line voltages from phase voltages (if needed): Vab=3⋅Van∠30°\mathbf{V}_{ab} = \sqrt{3}\cdot V_{an}\angle30°
  • This method reduces 3-phase analysis to a single-phase problem.
  • Only one phase is needed to solve the entire system due to symmetry and balance.
  • Always confirm phase sequence (abc vs. acb) before applying angles.

Insert Figure 10 here: Balanced Y-Y diagram
Insert Figure 11 here: Phasor diagram
Insert Figure 12 here: Single-phase equivalent

Balanced Wye-Delta (Y-Δ) Connection

🧠 What It Is

  • A Balanced Y-Δ system consists of a Wye-connected (Y) source supplying power to a Delta-connected (Δ) load.
  • Still assumes positive sequence (abc).
  • This configuration introduces a difference between line current and phase current on the load side.

⚙️ Key Terms

TermMeaning
ZΔZ_\DeltaImpedance per phase in the Δ-connected load
ZYZ_YEquivalent per-phase impedance after Δ-to-Y conversion
Van,Vbn,Vcn\mathbf{V}_{an}, \mathbf{V}_{bn}, \mathbf{V}_{cn}Source phase voltages (line-to-neutral)
Vab,Vbc,Vca\mathbf{V}_{ab}, \mathbf{V}_{bc}, \mathbf{V}_{ca}Source line voltages (line-to-line)
IAB,IBC,ICA\mathbf{I}_{AB}, \mathbf{I}_{BC}, \mathbf{I}_{CA}Phase currents in the Δ load
Ia,Ib,Ic\mathbf{I}_a, \mathbf{I}_b, \mathbf{I}_cLine currents from the source to Δ load
ILI_LLine current magnitude
IpI_pPhase current magnitude

In a Y-Δ system:
Line current ≠ Phase current
But: IL=3⋅IpI_L=3⋅I_p

🔌 Voltage Relationships

Assume positive sequence (abc):

Van=Vp∠0∘Vbn=Vp∠−120∘Vcn=Vp∠+120∘

Line voltages (using vector subtraction):

Vab=Van−Vbn=3Vp∠30∘Vbc=Vbn−Vcn=3Vp∠−90∘Vca=Vcn−Van=3Vp∠150∘

🔁 Phase & Line Current Relationships

Phase Currents (in Δ load):

Each phase current flows across each leg of the Delta:

IAB=VABZΔIBC=VBCZΔICA=VCAZΔ

Line Currents (KCL at nodes):

Apply Kirchhoff's Current Law (KCL) to get line currents:

Ia=IAB−ICAIb=IBC−IABIc=ICA−IBC

From phasor relationships:

Ia=IAB⋅3∠−30∘

So:

🔗 Line current = 3\sqrt{3} × Phase current and lags by 30∘30^\circ

🔄 Delta-to-Wye Transformation (Optional Trick)

To simplify the circuit, transform the Delta load into a Y equivalent:

ZY=ZΔ3\mathbf{Z}_Y=\frac{\mathbf{Z}_\Delta}{3}

Now it's a standard Y-Y system, and you can:

  • Use single-phase equivalent analysis

  • Solve for line current as:

    Ia=VanZY

Then:

  • Phase current:

    IAB=13⋅Ia∠+30∘

🪜 Step-by-Step Analysis Procedure

How to Analyze a Balanced Y-Δ Circuit

  1. Start with the source voltages: write the three phase voltages Van,Vbn,Vcn\mathbf{V}_{an}, \mathbf{V}_{bn}, \mathbf{V}_{cn}.

  2. Find the line voltages using:

    Vab=Van−Vbn,etc.

  3. Calculate phase currents in Δ:

    IAB=VABZΔ,etc.

  4. Use KCL to find line currents:

    Ia=IAB−ICA,etc.

  5. Optionally, transform Δ to Y if it simplifies the analysis:

    ZY=ZΔ3

🧭 Final Notes

  • Line currents are larger than phase currents.

  • Phase current leads line current by 30∘30^\circ.

  • Using the Δ-to-Y transformation simplifies analysis a lot, especially in exams.


Let me know if you want the diagram (e.g. from Figure 13 or 14) included as an image placeholder like:

![Figure 13: Balanced Y-Δ connection](insert-image-here)

Balanced Delta-Wye (Δ-Y) Connection

🧠 What It Is

  • A Balanced Δ-Y system is when the source is Delta-connected and the load is Wye-connected.
  • This setup is very common in power transmission and distribution systems.
  • The delta source can be converted into a wye equivalent to simplify analysis → turns it into a Y-Y system.

⚙️ Key Terms

TermMeaning
Z_sSource impedance per delta leg
Z_lLine impedance (between source and load)
Z_LLoad impedance per phase (in wye)
ZYZ_YTotal impedance per phase (as seen by the load)
Vab,Vbc,VcaV_{ab},V_{bc},V_{ca}Source line/phase voltages (Delta = line = phase)
Van,Vbn,VcnV_{an},V_{bn},V_{cn}Load phase voltages (line-to-neutral)
Ia,Ib,Ic\mathbf{I}_a,\mathbf{I}_b,\mathbf{I}_cLine currents feeding the wye load

In Delta connection:
Line Voltage = Phase Voltage

In Wye load:
Line Current = Phase Current


🔁 Delta to Wye Source Conversion

To simplify analysis:

  • Convert the delta source to an equivalent wye source.
  • Use this identity:
Van=Vab3∠(−30∘)V_{an} = \frac{V_{ab}}{\sqrt{3}}\angle(-30^\circ)
From DeltaTo Equivalent Wye
VabV_{ab}Van=Vab3∠(−30∘)V_{an} = \frac{V_{ab}}{\sqrt{3}}\angle(-30^\circ)
ZsZ_s per delta legZs3\frac{Z_s}{3} per wye leg

Once transformed, just use

Y-Y analysis methods as usual.


⚡ Relationship Between Voltages

Assuming abc sequence:

Vab=Vp∠0∘Vbc=Vp∠−120∘Vca=Vp∠+120∘\begin{aligned} \mathbf{V}_{ab} &= V_p\angle0^\circ \\ \mathbf{V}_{bc} &= V_p\angle-120^\circ \\ \mathbf{V}_{ca} &= V_p\angle+120^\circ \\ \end{aligned}

After conversion:

Van=Vp3∠−30∘Vbn=Vp3∠−150∘Vcn=Vp3∠+90∘\begin{aligned} \mathbf{V}_{an} &= \frac{V_p}{\sqrt{3}} \angle -30^\circ \\ \mathbf{V}_{bn} &= \frac{V_p}{\sqrt{3}} \angle -150^\circ \\ \mathbf{V}_{cn} &= \frac{V_p}{\sqrt{3}} \angle +90^\circ \\ \end{aligned}

🔌 Line Currents Derivation (Without Delta-Wye conversion)

Apply KVL in loop aANBba:

−ZYIa+ZYIb=Vab⇒ZY(Ia−Ib)=Vab-Z_Y I_a + Z_Y I_b = V_{ab} \Rightarrow Z_Y (I_a - I_b) = V_{ab}

Assume abc sequence ⇒ Ib=Ia∠−120∘I_b = I_a \angle -120^\circ, then:

Ia−Ib=Ia(1−∠−120∘)=Ia3∠30∘I_a - I_b = I_a(1 - \angle -120^\circ) = I_a \sqrt{3}\angle30^\circ

Solve:

Ia=Vab3ZY∠−30∘I_a = \frac{V_{ab}}{\sqrt{3}Z_Y} \angle -30^\circ

🔍 Step-by-Step Analysis Procedure

Use this procedure if converting Delta to Wye:

  1. Transform Delta source to an equivalent Wye:

    • Van=Vab3∠(−30∘)V_{an} = \frac{V_{ab}}{\sqrt{3}}\angle(-30^\circ)
    • ZsZ_s becomes Zs3\frac{Z_s}{3}
  2. Draw the single-phase equivalent circuit (typically phase A).

  3. Solve for the line/phase current:

    Ia=VanZY\mathbf{I}_a = \frac{\mathbf{V}_{an}}{Z_Y}
  4. Extend solution to other phases using 120° phase shifts:

    Ib=Ia∠−120∘Ic=Ia∠+120∘\mathbf{I}_b = \mathbf{I}_a \angle -120^\circ \quad \mathbf{I}_c = \mathbf{I}_a \angle +120^\circ

Takeaways

  • Transforming Delta to Wye makes analysis simpler.
  • In Δ-Y:
    • Voltage transformation involves 3\sqrt{3} scaling and -30° phase shift.
    • Current calculation can follow delta loop KVL or convert to Y-Y for standard method.

Balanced Delta-Delta (Δ-Δ) Connection

🧠 What It Is

  • A Balanced Δ-Δ system means both source and load are Delta-connected and balanced.
  • It's less common than Y-Y or Y-Δ, but useful for specific transformer configurations or motor loads.
  • If needed, you can always convert Δ to Y (for either source or load) to simplify the analysis.

✅ Many problems can be reduced to Y-Y format by using Δ-to-Y transformation.


⚙️ Key Concepts and Terms

TermMeaning
Z_ΔLoad impedance per Δ leg (line-to-line impedance)
IAB,IBC,ICAI_{AB}, I_{BC}, I_{CA}Phase currents flowing in the Δ branches
Ia,Ib,IcI_a, I_b, I_cLine currents, connected to each corner of the Δ
VAB,VBC,VCAV_{AB}, V_{BC}, V_{CA}Line voltages = phase voltages in Δ system

🔁 Relationship Between Line and Phase Currents

  • In Δ, phase voltages = line voltages directly:
VAB=Vab,VBC=Vbc,VCA=VcaV_{AB} = V_{ab}, \quad V_{BC} = V_{bc}, \quad V_{CA} = V_{ca}
  • Phase currents:
IAB=VABZΔ,IBC=VBCZΔ,ICA=VCAZΔI_{AB} = \frac{V_{AB}}{Z_\Delta}, \quad I_{BC} = \frac{V_{BC}}{Z_\Delta}, \quad I_{CA} = \frac{V_{CA}}{Z_\Delta}
  • Line currents (from KCL):
Ia=IAB−ICAIb=IBC−IABIc=ICA−IBC\begin{aligned} I_a &= I_{AB} - I_{CA} \\ I_b &= I_{BC} - I_{AB} \\ I_c &= I_{CA} - I_{BC} \end{aligned}
  • Magnitude relationship:
IL=3⋅Iphase,andLine current lags phase current by 30∘\boxed{I_L = \sqrt{3} \cdot I_{phase}}, \quad \text{and} \quad \text{Line current lags phase current by } 30^\circ

🔄 Δ-to-Y Transformation (For Easier Analysis)

  • To simplify the analysis, convert both Δ source/load to Y:
ZY=ZΔ3Z_Y = \frac{Z_\Delta}{3}
  • Once transformed to Y-Y:
    • Use normal Y-Y analysis like in your previous notes.
    • Solve for single-phase equivalent.
    • Then extend by 120∘120^\circ rotation.

⚠️ Don't forget to convert both the source and the load to Y if the problem allows it, to simplify the system into a single-phase equivalent model.


🧪 Step-by-Step Analysis (Optional Shortcut via Y-Y)

  1. Convert Delta load to equivalent Wye:

    ZY=ZΔ3Z_Y = \frac{Z_\Delta}{3}
  2. If needed, convert source to Wye too.

  3. Draw single-phase equivalent circuit (usually for phase A).

  4. Solve using:

    Ia=VanZY+Zline+ZsI_a = \frac{V_{an}}{Z_Y + Z_{line} + Z_s}
  5. Extend solution to IbI_b and IcI_c by rotating −120∘-120^\circ and +120∘+120^\circ.

  6. Convert back (if necessary) to get actual Δ current values.


Remember:

  • In Δ-Δ: line voltage = phase voltage
  • Line current is larger than phase current by 3\sqrt{3}
  • Always confirm phase sequence and angles before solving

![Insert textbook figure here if needed]