Series and parallel resistor circuit examples with formulas and calculated total resistance values.
Diagrams showing series and parallel resistor circuits with calculations for equivalent resistance.
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Step-by-step solution for: Physics - Equivalent Resistance Practice - 1 page worksheet ...
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Show Answer Key & Explanations
Step-by-step solution for: Physics - Equivalent Resistance Practice - 1 page worksheet ...
To solve the problem, we need to calculate the equivalent resistance for each of the given circuits. Let's go through each case step by step.
---
The resistors are connected in series. The formula for the equivalent resistance \( R_{\text{eq}} \) in a series circuit is:
\[
R_{\text{eq}} = R_1 + R_2 + R_3 + \cdots
\]
Given:
- \( R_1 = 8 \, \Omega \)
- \( R_2 = 2 \, \Omega \)
- \( R_3 = 4 \, \Omega \)
\[
R_{\text{eq}} = 8 + 2 + 4 = 14 \, \Omega
\]
Answer for Case 1:
\[
\boxed{14 \, \Omega}
\]
---
The resistors are connected in parallel. The formula for the equivalent resistance \( R_{\text{eq}} \) in a parallel circuit is:
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \cdots
\]
Given:
- \( R_1 = 4 \, \Omega \)
- \( R_2 = 6 \, \Omega \)
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{4} + \frac{1}{6}
\]
Find a common denominator (which is 12):
\[
\frac{1}{R_{\text{eq}}} = \frac{3}{12} + \frac{2}{12} = \frac{5}{12}
\]
Thus,
\[
R_{\text{eq}} = \frac{12}{5} = 2.4 \, \Omega
\]
Answer for Case 2:
\[
\boxed{2.4 \, \Omega}
\]
---
The circuit consists of a combination of series and parallel connections. We will simplify it step by step.
#### Step 1: Simplify the parallel section
The two resistors in parallel are:
- \( R_1 = 2 \, \Omega \)
- \( R_2 = 4 \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{parallel}}} = \frac{1}{2} + \frac{1}{4}
\]
Find a common denominator (which is 4):
\[
\frac{1}{R_{\text{parallel}}} = \frac{2}{4} + \frac{1}{4} = \frac{3}{4}
\]
Thus,
\[
R_{\text{parallel}} = \frac{4}{3} \, \Omega
\]
#### Step 2: Add the series resistor
The simplified parallel resistance \( R_{\text{parallel}} = \frac{4}{3} \, \Omega \) is now in series with another resistor \( R_3 = 8 \, \Omega \).
Using the series formula:
\[
R_{\text{eq}} = R_{\text{parallel}} + R_3 = \frac{4}{3} + 8
\]
Convert 8 to a fraction with a denominator of 3:
\[
R_{\text{eq}} = \frac{4}{3} + \frac{24}{3} = \frac{28}{3} \, \Omega
\]
Answer for Case 3:
\[
\boxed{\frac{28}{3} \, \Omega}
\]
---
This circuit involves multiple series and parallel combinations. We will simplify it step by step.
#### Step 1: Simplify the inner parallel section
The two resistors in parallel are:
- \( R_1 = 4 \, \Omega \)
- \( R_2 = 6 \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{parallel}}} = \frac{1}{4} + \frac{1}{6}
\]
Find a common denominator (which is 12):
\[
\frac{1}{R_{\text{parallel}}} = \frac{3}{12} + \frac{2}{12} = \frac{5}{12}
\]
Thus,
\[
R_{\text{parallel}} = \frac{12}{5} \, \Omega
\]
#### Step 2: Add the series resistor
The simplified parallel resistance \( R_{\text{parallel}} = \frac{12}{5} \, \Omega \) is now in series with another resistor \( R_3 = 8 \, \Omega \).
Using the series formula:
\[
R_{\text{series}} = R_{\text{parallel}} + R_3 = \frac{12}{5} + 8
\]
Convert 8 to a fraction with a denominator of 5:
\[
R_{\text{series}} = \frac{12}{5} + \frac{40}{5} = \frac{52}{5} \, \Omega
\]
#### Step 3: Simplify the outer parallel section
The two resistors in parallel are:
- \( R_1 = 2 \, \Omega \)
- \( R_2 = \frac{52}{5} \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{1}{\frac{52}{5}}
\]
Simplify \( \frac{1}{\frac{52}{5}} \):
\[
\frac{1}{\frac{52}{5}} = \frac{5}{52}
\]
Thus,
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{5}{52}
\]
Find a common denominator (which is 52):
\[
\frac{1}{R_{\text{eq}}} = \frac{26}{52} + \frac{5}{52} = \frac{31}{52}
\]
Thus,
\[
R_{\text{eq}} = \frac{52}{31} \, \Omega
\]
Answer for Case 4:
\[
\boxed{\frac{52}{31} \, \Omega}
\]
---
1. \(\boxed{14 \, \Omega}\)
2. \(\boxed{2.4 \, \Omega}\)
3. \(\boxed{\frac{28}{3} \, \Omega}\)
4. \(\boxed{\frac{52}{31} \, \Omega}\)
---
Case 1: Series Circuit
The resistors are connected in series. The formula for the equivalent resistance \( R_{\text{eq}} \) in a series circuit is:
\[
R_{\text{eq}} = R_1 + R_2 + R_3 + \cdots
\]
Given:
- \( R_1 = 8 \, \Omega \)
- \( R_2 = 2 \, \Omega \)
- \( R_3 = 4 \, \Omega \)
\[
R_{\text{eq}} = 8 + 2 + 4 = 14 \, \Omega
\]
Answer for Case 1:
\[
\boxed{14 \, \Omega}
\]
---
Case 2: Parallel Circuit
The resistors are connected in parallel. The formula for the equivalent resistance \( R_{\text{eq}} \) in a parallel circuit is:
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \cdots
\]
Given:
- \( R_1 = 4 \, \Omega \)
- \( R_2 = 6 \, \Omega \)
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{4} + \frac{1}{6}
\]
Find a common denominator (which is 12):
\[
\frac{1}{R_{\text{eq}}} = \frac{3}{12} + \frac{2}{12} = \frac{5}{12}
\]
Thus,
\[
R_{\text{eq}} = \frac{12}{5} = 2.4 \, \Omega
\]
Answer for Case 2:
\[
\boxed{2.4 \, \Omega}
\]
---
Case 3: Mixed Circuit (Series and Parallel)
The circuit consists of a combination of series and parallel connections. We will simplify it step by step.
#### Step 1: Simplify the parallel section
The two resistors in parallel are:
- \( R_1 = 2 \, \Omega \)
- \( R_2 = 4 \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{parallel}}} = \frac{1}{2} + \frac{1}{4}
\]
Find a common denominator (which is 4):
\[
\frac{1}{R_{\text{parallel}}} = \frac{2}{4} + \frac{1}{4} = \frac{3}{4}
\]
Thus,
\[
R_{\text{parallel}} = \frac{4}{3} \, \Omega
\]
#### Step 2: Add the series resistor
The simplified parallel resistance \( R_{\text{parallel}} = \frac{4}{3} \, \Omega \) is now in series with another resistor \( R_3 = 8 \, \Omega \).
Using the series formula:
\[
R_{\text{eq}} = R_{\text{parallel}} + R_3 = \frac{4}{3} + 8
\]
Convert 8 to a fraction with a denominator of 3:
\[
R_{\text{eq}} = \frac{4}{3} + \frac{24}{3} = \frac{28}{3} \, \Omega
\]
Answer for Case 3:
\[
\boxed{\frac{28}{3} \, \Omega}
\]
---
Case 4: Complex Mixed Circuit
This circuit involves multiple series and parallel combinations. We will simplify it step by step.
#### Step 1: Simplify the inner parallel section
The two resistors in parallel are:
- \( R_1 = 4 \, \Omega \)
- \( R_2 = 6 \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{parallel}}} = \frac{1}{4} + \frac{1}{6}
\]
Find a common denominator (which is 12):
\[
\frac{1}{R_{\text{parallel}}} = \frac{3}{12} + \frac{2}{12} = \frac{5}{12}
\]
Thus,
\[
R_{\text{parallel}} = \frac{12}{5} \, \Omega
\]
#### Step 2: Add the series resistor
The simplified parallel resistance \( R_{\text{parallel}} = \frac{12}{5} \, \Omega \) is now in series with another resistor \( R_3 = 8 \, \Omega \).
Using the series formula:
\[
R_{\text{series}} = R_{\text{parallel}} + R_3 = \frac{12}{5} + 8
\]
Convert 8 to a fraction with a denominator of 5:
\[
R_{\text{series}} = \frac{12}{5} + \frac{40}{5} = \frac{52}{5} \, \Omega
\]
#### Step 3: Simplify the outer parallel section
The two resistors in parallel are:
- \( R_1 = 2 \, \Omega \)
- \( R_2 = \frac{52}{5} \, \Omega \)
Using the parallel formula:
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{1}{\frac{52}{5}}
\]
Simplify \( \frac{1}{\frac{52}{5}} \):
\[
\frac{1}{\frac{52}{5}} = \frac{5}{52}
\]
Thus,
\[
\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{5}{52}
\]
Find a common denominator (which is 52):
\[
\frac{1}{R_{\text{eq}}} = \frac{26}{52} + \frac{5}{52} = \frac{31}{52}
\]
Thus,
\[
R_{\text{eq}} = \frac{52}{31} \, \Omega
\]
Answer for Case 4:
\[
\boxed{\frac{52}{31} \, \Omega}
\]
---
Final Answers:
1. \(\boxed{14 \, \Omega}\)
2. \(\boxed{2.4 \, \Omega}\)
3. \(\boxed{\frac{28}{3} \, \Omega}\)
4. \(\boxed{\frac{52}{31} \, \Omega}\)
Parent Tip: Review the logic above to help your child master the concept of series parallel resistor worksheet.