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Introduction to Marine Engineering

Subsection 4.3.2 Parallel Circuit

In a parallel circuit, the components are connected between the same two points, creating a separate current path for each component. Parallel components all use the same power supply but can be turned on and off independently.
Figure 4.3.3. Three resistors in parallel
The key characteristics parallel circuits are:
  • The same voltage is applied to all parallel components.
  • The current through each component may be different, but the total current is the sum of the currents through each component.
  • The total resistance of a parallel circuit containing \(n\) branches is given by this formula
    \begin{equation} R_t = \frac{1}{1/R_1 + 1/R_2 + 1/R_3 + ... 1/R_n}\text{.}\tag{4.3.1} \end{equation}

Example 4.3.4. Parallel resistors.

Consider the series circuit in Figure 4.3.3.
If the battery supplies 100 V, and the resistors are \(R_1 = 100\ \Omega\text{,}\) \(R_2 = 200\ \Omega\text{,}\) and\(R_3= 500\ \Omega\text{,}\) determine
  1. The total current \(I\) in the circuit, and
  2. The total current if branch 3 is turned off by opening the third switch.
Answer.
For all three branches in operation: I = 1.7 A.
For just the first two branches I = 1.5 A.
Solution 1.
The current in each branch may be found using Ohms Law
\begin{equation*} I = E/R\text{.} \end{equation*}
Use Ohm’s Law \(I = E/R\) to calculate the current through each resistor.
\begin{align*} I_1 \amp= E/R_1 = \frac{100 \text{ V}}{100\ \Omega} = 1.0 \text{ A}\\ I_2 \amp= E/R_2 = \frac{100 \text{ V}}{200\ \Omega}= 0.5 \text{ A}\\ I_3 \amp= E/R_3 = \frac{100 \text{ V}}{500\ \Omega}= 0.2 \text{ A} \end{align*}
The total current for all three branches is
\begin{equation*} I = I_1 + I_2 +I_3 = 1.7 \text{ A} \end{equation*}
When the switch in branch 3 is opened current \(I_3\) drops to zero, so the total current drops to 1.5 A
Solution 2.
An alternate solution method is to first find the equivalent resistance using (4.3.1), then use that resistance to find the current.
For all three resistors
\begin{equation*} R_t = \frac{1}{\frac{1}{100}+\frac{1}{200} + \frac{1}{500}} = 58.8\ \Omega\text{,} \end{equation*}
and the corresponding current is
\begin{equation*} I =\frac{E}{R_t}= \frac{100 \text{ V}}{58.8\ \Omega} = 1.7 \text{ A} \end{equation*}
Repeating the calculations for the first two resistors only we get
\begin{gather*} R_t = \frac{1}{\frac{1}{100}+\frac{1}{200}} = 66.7\ \Omega\\ I = \frac{E}{R_t} = \frac{100 \text{ V}}{66.7\ \Omega} = 1.5 \text{ A} \end{gather*}

Example 4.3.5. Series-Parallel resistors.

For the series-parallel circuit below, determine the total current \(I\) if the battery supplies 120 V, and the resistors are \(R_1 = 100\ \Omega\text{,}\) \(R_2 = 200\ \Omega\text{,}\) and \(R_3= 500\ \Omega\text{.}\)
Answer.
I = 0.494 A = 494 mA.
Solution.
The system can be thought of as resistor \(R_1\) in series with the parallel combination of resistors \(R_2\) and \(R_3\text{.}\) The total resistance of this combination is
\begin{align*} R_t \amp= R_1 + \frac{1}{\frac{1}{R_2}+\frac{1}{R_3}}\\ \amp= 100 + \frac{1}{\frac{1}{200}+\frac{1}{500}}\\ \amp= 242.9\ \Omega \end{align*}
Applying Ohm’s Law with this resistance gives the current
\begin{equation*} I = E/R_t = \frac{120 \text{ V}}{242.9\ \Omega} = 0.494\text{ A} \end{equation*}