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In a series circuit, all components are connected one after another, allowing the same electric current to flow through each component sequentially. This means the overall resistance in the circuit is simply the sum of individual resistances. When resistors are connected in series, the total resistance can be calculated using the formula:

• \( R_{total} = R_1 + R_2 + R_3 + ... + R_n \)

For example, if three identical resistors each have a resistance \( R \), the total resistance is given by \( R_{total} = 3R \). The voltage drop across the entire circuit distributes among the three resistors, but they all carry the same current. As a result, the power dissipated can be calculated by the following formula:

• \( P = \frac{V^2}{R_{total}} \)

A parallel circuit offers multiple different paths for the electric current to flow. If one path is obstructed or broken, the others can continue to function. In contrast to series circuits, the total resistance in a parallel circuit decreases. It can be determined using the reciprocal formula:

• \( \frac{1}{R_{total}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + ... + \frac{1}{R_n} \)

For three identical resistors connected in parallel, the formula becomes

• \( \frac{1}{R_{total}} = \frac{1}{R} + \frac{1}{R} + \frac{1}{R} = \frac{3}{R} \)

Simplifying this equation results in the total resistance:

• \( R_{total} = \frac{R}{3} \)

A key feature of a parallel circuit is that each branch receives the same voltage across it, making it different from series circuits where the voltage is divided across components.

Power dissipation refers to the process by which electrical energy is converted into thermal energy or heat within a circuit, often across resistors. It's a critical factor in both series and parallel circuits. Power dissipation is governed by the formula:

• \( P = VI \)
• \( P = I^2R \) (for circuits with a known current)
• \( P = \frac{V^2}{R} \) (for circuits with a known voltage)

In a series circuit, when resistors are all identical and organized in a line, the power can be calculated as \( P = \frac{V^2}{3R} \), showing how the power dissipates over the combined resistance. In parallel circuits, power dissipation changes since each pathway supports the same voltage, and the total power dissipation increases as more parallel paths allow for more current flow, thus more energy dissipation.

Calculating resistance is a crucial step in analyzing both series and parallel circuits. For series circuits, resistance is straightforward, as you just sum up the individual resistances. However, for parallel circuits, it becomes necessary to use the reciprocal relation for accurate calculations.

• Series: \( R_{total} = R_1 + R_2 + R_3 + ... + R_n \)
• Parallel: \( \frac{1}{R_{total}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + ... \)

Analyzing the given problem where each resistor has the same resistance \( R \), the equivalent resistance for three resistors in series is \( 3R \), while for parallel, it's \( \frac{R}{3} \). This distinction is crucial for determining how circuits will carry current and how they will respond to electrical power, especially under a fixed voltage. Computing these resistances accurately helps in predicting how much power will dissipate across such configurations.