What is the relationship between resistance connected in delta and equivalent star system?
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In electrical engineering, particularly in three-phase systems, the **Delta (Δ)** and **Star (Y)** connections refer to different ways of connecting resistances (or impedances) in a circuit. Understanding the relationship between these two configurations is crucial for analyzing three-phase circuits. Here's a detailed explanation of the relationship between resistances connected in delta and their equivalent star system:

### Basic Definitions

1. **Delta Connection (Δ)**:
   - In a delta connection, the components (resistances) are connected in a loop (triangle shape). Each resistance connects to two other resistances.
   - For example, if we have three resistances \( R_{A}, R_{B}, R_{C} \), they would connect at points A, B, and C forming a triangle.

2. **Star Connection (Y)**:
   - In a star connection, all components connect to a common central point (the star point). Each resistance connects from this central point to a terminal.
   - Using the same resistances \( R_{A}, R_{B}, R_{C} \), each would connect to a central node, forming a “Y” shape.

### Mathematical Relationship

To establish the relationship between the delta and star configurations, we can derive formulas to convert between the two systems.

#### Conversion from Delta to Star

Given resistances \( R_A \), \( R_B \), and \( R_C \) in a delta configuration, the equivalent resistances \( R_{A}' \), \( R_{B}' \), and \( R_{C}' \) in the star configuration can be calculated as follows:

\[
R_{A}' = \frac{R_A R_B}{R_A + R_B + R_C}
\]

\[
R_{B}' = \frac{R_B R_C}{R_A + R_B + R_C}
\]

\[
R_{C}' = \frac{R_C R_A}{R_A + R_B + R_C}
\]

- Here, \( R_{A}' \), \( R_{B}' \), and \( R_{C}' \) are the resistances in the star configuration.

#### Conversion from Star to Delta

Conversely, if you have resistances in a star configuration, the equivalent resistances in a delta configuration can be calculated using:

\[
R_A = \frac{R_{A}' R_{B}'}{R_{A}' + R_{B}' + R_{C}'}
\]

\[
R_B = \frac{R_{B}' R_{C}'}{R_{A}' + R_{B}' + R_{C}'}
\]

\[
R_C = \frac{R_{C}' R_{A}'}{R_{A}' + R_{B}' + R_{C}'}
\]

### Implications of the Relationship

1. **Voltage and Current Relationships**:
   - In a delta connection, the phase voltage is equal to the line voltage, while the line current is divided among the phases.
   - In a star connection, the phase voltage is the line voltage divided by \( \sqrt{3} \), and the line current is equal to the phase current.

2. **Power Calculations**:
   - The total power in both configurations can be analyzed by converting from one to the other. The relationships between line and phase voltages and currents significantly affect power calculations.

3. **Impedance Matching**:
   - Knowing how to convert between delta and star configurations helps in impedance matching in circuits, ensuring maximum power transfer.

### Example

Let’s consider an example where:

- Delta resistances: \( R_A = 30 \, \Omega \), \( R_B = 20 \, \Omega \), \( R_C = 10 \, \Omega \).

To find the equivalent star resistances:

1. Calculate \( R_{A}' \):

\[
R_{A}' = \frac{30 \times 20}{30 + 20 + 10} = \frac{600}{60} = 10 \, \Omega
\]

2. Calculate \( R_{B}' \):

\[
R_{B}' = \frac{20 \times 10}{30 + 20 + 10} = \frac{200}{60} \approx 3.33 \, \Omega
\]

3. Calculate \( R_{C}' \):

\[
R_{C}' = \frac{10 \times 30}{30 + 20 + 10} = \frac{300}{60} = 5 \, \Omega
\]

So, the equivalent star resistances are \( R_{A}' = 10 \, \Omega \), \( R_{B}' \approx 3.33 \, \Omega \), and \( R_{C}' = 5 \, \Omega \).

### Conclusion

The relationship between delta and star connected resistances is fundamental in circuit analysis, allowing engineers to easily switch between configurations for calculations. By using the derived formulas, one can determine the equivalent resistances in either configuration, facilitating the understanding of the electrical behavior of three-phase systems. This conversion is particularly useful in power distribution, load balancing, and circuit design.
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The relationship between resistances connected in a **Delta (Δ)** configuration and an **equivalent Star (Y)** configuration is important in electrical circuit analysis, especially when simplifying complex resistor networks.

### 1. **Delta (Δ) Configuration**:
In a Delta configuration, the resistors are connected in a triangle-like structure. Each resistor connects two nodes, with three resistors forming the three sides of the triangle.

Let the resistances in the Delta configuration be:

- \( R_{AB} \): the resistance between nodes A and B,
- \( R_{BC} \): the resistance between nodes B and C,
- \( R_{CA} \): the resistance between nodes C and A.

### 2. **Star (Y) Configuration**:
In a Star configuration, the resistors are connected in a Y-shaped structure. Here, three resistors have a common central node, with each resistor connecting the central node to one of the outer nodes (A, B, or C).

Let the resistances in the Star configuration be:

- \( R_A \): the resistance between the central node and node A,
- \( R_B \): the resistance between the central node and node B,
- \( R_C \): the resistance between the central node and node C.

### 3. **Conversion Between Delta and Star**:

To convert a Delta (Δ) network into an equivalent Star (Y) network, we use specific formulas to ensure the electrical properties (like the total resistance between any two points) are preserved.

#### **Star to Delta Conversion**:

If you want to convert the Star resistances \( R_A \), \( R_B \), and \( R_C \) into the equivalent Delta resistances \( R_{AB} \), \( R_{BC} \), and \( R_{CA} \), the following relationships hold:

\[
R_{AB} = \frac{R_A R_B + R_B R_C + R_C R_A}{R_C}
\]
\[
R_{BC} = \frac{R_A R_B + R_B R_C + R_C R_A}{R_A}
\]
\[
R_{CA} = \frac{R_A R_B + R_B R_C + R_C R_A}{R_B}
\]

These equations allow us to calculate the equivalent Delta resistances from a Star configuration.

#### **Delta to Star Conversion**:

To convert the Delta resistances \( R_{AB} \), \( R_{BC} \), and \( R_{CA} \) into equivalent Star resistances \( R_A \), \( R_B \), and \( R_C \), we use the following formulas:

\[
R_A = \frac{R_{AB} R_{CA}}{R_{AB} + R_{BC} + R_{CA}}
\]
\[
R_B = \frac{R_{AB} R_{BC}}{R_{AB} + R_{BC} + R_{CA}}
\]
\[
R_C = \frac{R_{BC} R_{CA}}{R_{AB} + R_{BC} + R_{CA}}
\]

These equations allow us to calculate the equivalent Star resistances from a Delta configuration.

### 4. **Explanation of the Relationship**:

- **Preservation of Equivalent Resistance**: The conversion between Delta and Star configurations is designed to ensure that the resistance between any two external nodes (A, B, or C) remains the same in both configurations.
  
- **Reduction of Complex Circuits**: Often, a circuit with resistors in Delta configuration is harder to analyze. By converting it to a Star configuration, the analysis becomes easier, particularly when dealing with series and parallel combinations.

- **Useful in AC Networks**: This relationship is extensively used in AC power systems, especially in the analysis of three-phase systems where loads can be connected in either Delta or Star configuration. The conversion simplifies analysis by allowing engineers to compare systems and solve circuit problems more easily.

### 5. **Example Calculation**:

Consider a Delta network with:

- \( R_{AB} = 30 \, \Omega \)
- \( R_{BC} = 60 \, \Omega \)
- \( R_{CA} = 90 \, \Omega \)

To find the equivalent Star resistances \( R_A \), \( R_B \), and \( R_C \), we can use the Delta to Star conversion formulas:

\[
R_A = \frac{R_{AB} R_{CA}}{R_{AB} + R_{BC} + R_{CA}} = \frac{30 \times 90}{30 + 60 + 90} = \frac{2700}{180} = 15 \, \Omega
\]

\[
R_B = \frac{R_{AB} R_{BC}}{R_{AB} + R_{BC} + R_{CA}} = \frac{30 \times 60}{30 + 60 + 90} = \frac{1800}{180} = 10 \, \Omega
\]

\[
R_C = \frac{R_{BC} R_{CA}}{R_{AB} + R_{BC} + R_{CA}} = \frac{60 \times 90}{30 + 60 + 90} = \frac{5400}{180} = 30 \, \Omega
\]

Thus, the equivalent Star resistances are \( R_A = 15 \, \Omega \), \( R_B = 10 \, \Omega \), and \( R_C = 30 \, \Omega \).

### Conclusion:
The relationship between Delta and Star resistances is crucial for simplifying circuits and analyzing electrical networks. The ability to convert between these configurations helps in maintaining the same overall resistance between nodes, making it easier to solve complex problems in both DC and AC circuits.
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