Resistors in Series

Understand series circuits and how to calculate total resistance, current, and voltage distribution

Overview

In a series connection, multiple resistors are connected in a line, so the current flows through each resistor in sequence. The same current flows through all resistors in a series circuit.

Series resistors circuit diagram
Characteristic:

The same current flows through all resistors, but the voltage divides across them proportionally to their resistance values. This is opposite to parallel circuits.

Total Resistance

In a series circuit, the total resistance is simply the sum of all individual resistances.

Key Principle:

Resistances add directly in series. Adding more resistors always increases the total resistance.

\(\displaystyle R_{\text{total}} = R_1 + R_2 + R_3 + \ldots\)
Key observation

The total resistance in a series circuit is always greater than any individual resistance. Each resistor adds to the total resistance.

Current in Series Circuit

The same current flows through all resistors in a series circuit. Using Ohm's Law, we can calculate this current from the total voltage and total resistance.

Current Rule:

The total current through all resistors is identical:

\(\displaystyle I_{\text{total}} = I_1 = I_2 = I_3 = \ldots\)

Using Ohm's Law with total values:

\(\displaystyle I = \frac{U_{\text{total}}}{R_{\text{total}}}\)

Voltage Division in Series

In a series circuit, the total voltage divides across the individual resistors. The voltage distribution is proportional to the resistance values.

Voltage Sum Rule

The total voltage is the sum of the individual voltages:

\(\displaystyle U_{\text{total}} = U_1 + U_2 + U_3 + \ldots\)

Voltage Divider Principle

The voltage across each resistor is proportional to its resistance. The ratio of voltages equals the ratio of resistances:

\(\displaystyle \frac{U_{\text{total}}}{R_{\text{total}}} = \frac{U_1}{R_1} = \frac{U_2}{R_2} = \frac{U_3}{R_3}\)

Individual Voltage Formulas

The voltage across a specific resistor can be calculated in two ways:

Method 1: Using Current
\(\displaystyle U_1 = R_1 \cdot I\)
Method 2: Using Ratio
\(\displaystyle U_1 = \frac{R_1 \cdot U_{\text{total}}}{R_{\text{total}}}\)

Worked Example

Calculate Series Resistor Circuit

Given:

  • \(R_1 = 20\,\Omega\)
  • \(R_2 = 40\,\Omega\)
  • \(R_3 = 55\,\Omega\)
  • \(U_{\text{total}} = 230\,\text{V}\)
Series resistors example circuit

Step 1: Calculate total resistance

\(\displaystyle R_{\text{total}} = R_1 + R_2 + R_3 = 20 + 40 + 55 = 115\,\Omega\)

Step 2: Calculate total current

\(\displaystyle I = \frac{U_{\text{total}}}{R_{\text{total}}} = \frac{230}{115} = 2\,\text{A}\)

Step 3: Calculate individual voltages

Voltage across \(R_1\):

Method 1: \(\displaystyle U_1 = R_1 \cdot I = 20 \cdot 2 = 40\,\text{V}\)

Method 2: \(\displaystyle U_1 = \frac{R_1 \cdot U_{\text{total}}}{R_{\text{total}}} = \frac{20 \cdot 230}{115} = 40\,\text{V}\)

Voltage across \(R_2\):

Method 1: \(\displaystyle U_2 = R_2 \cdot I = 40 \cdot 2 = 80\,\text{V}\)

Method 2: \(\displaystyle U_2 = \frac{R_2 \cdot U_{\text{total}}}{R_{\text{total}}} = \frac{40 \cdot 230}{115} = 80\,\text{V}\)

Voltage across \(R_3\):

Method 1: \(\displaystyle U_3 = R_3 \cdot I = 55 \cdot 2 = 110\,\text{V}\)

Method 2: \(\displaystyle U_3 = \frac{R_3 \cdot U_{\text{total}}}{R_{\text{total}}} = \frac{55 \cdot 230}{115} = 110\,\text{V}\)

Verification:

\(\displaystyle U_1 + U_2 + U_3 = 40 + 80 + 110 = 230\,\text{V}\) ✓

Summary: Series vs Parallel

Series Circuit
Resistance: \(R = R_1 + R_2 + \ldots\)
Current: Same everywhere
Voltage: Divides proportionally
Parallel Circuit
Resistance: \(\frac{1}{R} = \frac{1}{R_1} + \frac{1}{R_2} + \ldots\)
Current: Divides proportionally
Voltage: Same everywhere

Key Properties of Series Circuits

  • Same current flows through all resistors
  • Total resistance is sum of individual resistances
  • Total voltage is sum of individual voltages
  • Voltage divides proportionally to resistance values
  • Higher resistance resistor gets higher voltage drop
  • Total resistance is always greater than any individual resistor
  • If one component fails (opens), the entire circuit breaks


Resistors in Parallel
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