
Find the Norton equivalent circuit across A-B terminal for the circuit shown
Answer
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Hint: The Norton current I is the open circuit voltage divided by the resistance r across that terminal. The Norton resistance r across A-B with all voltage sources replaced by short circuit and all current sources replaced by open sources.
Complete step by step answer:
Note:
Norton and Thevenin theorems are used to solve the complex circuit questions. Thevenin's theorem can be applied while analyzing a circuit with dependent sources. In this case, all independent sources are turned off and the $R_{Th}$ is calculated by applying a current source or voltage source at the open terminal of the circuit. When using a voltage source, it can be assumed to be 1V for easy calculations.
Complete step by step answer:
Step 1: We have to find the load resistance. Load resistance is the resistance through which we have to find the Norton current. So here we have to find the current through A-B terminal so the load resistance is 10Ω.
$R_L$ = 10 Ω
Step 2: We will find Norton equivalent resistance ($R_n$) which will be equivalent to the resistance across A-B terminal. For this we will short circuit the voltage source and open circuit all the current source as shown in the figure. Equivalent resistance across the A-B terminal is $R_n$.
5 Ω and 10 Ω are in parallel with each other. Their equivalent is $R$,
$\dfrac{1}{R} = \dfrac{1}{5} + \dfrac{1}{{10}} $
$\Rightarrow \dfrac{1}{R} = \dfrac{{5 + 10}}{{10 \times 5}} $
$\Rightarrow \dfrac{1}{R} = \dfrac{{15}}{{50}} $
$\Rightarrow R = \dfrac{10}{3} $
Now this $R$ is in series with 3 Ω.
$R_n = \dfrac{{10}}{3}\Omega + 3\Omega $
$\Rightarrow R_n = \dfrac{{10 + 9}}{3}\Omega$
$\Rightarrow R_n = \dfrac{{19}}{{3}}\Omega $
STEP 3: Now we will find the Norton current which is equal to $I_n$.Norton current is the current which passes through A-B terminal
Both the 3 Ω resistance are parallel to each other so their effective resistance is
$\dfrac{1}{R} = \dfrac{1}{3} + \dfrac{1}{3} $
$\Rightarrow \dfrac{1}{R} = \dfrac{2}{3} $
$\Rightarrow R = \dfrac{3}{2} $
Now $R$ is in series with 5 Ω
$R = \dfrac{3}{2} + 5 $
$\Rightarrow R = \dfrac{13}{2}$
$\Rightarrow \text{CURRENT} = \dfrac{\text{VOLTAGE}}{\text{RESISTANCE}} $
$\Rightarrow I = \dfrac{{30}}{{\dfrac{{13}}{2}}} $
$\Rightarrow I = \dfrac{{30 \times 2}}{{13}} $
$\Rightarrow I = \dfrac{{60}}{{13}} $
Now this current will be equally
$I_n = \dfrac{{30}}{{13}}$
STEP 4: We will draw an equivalent circuit with all three $I_n , R_n$ and $R_l$ in parallel to each other.
$x = \dfrac{{R_n}}{{R_n + Rl}} \times I_n $
$\Rightarrow x = \dfrac{{\dfrac{{19}}{3}}}{{\dfrac{{19}}{3} + 10}} \times \dfrac{{30}}{{13}} $
$\therefore x = \dfrac{{19 \times 30}}{{49 \times 13}}A $
Norton and Thevenin theorems are used to solve the complex circuit questions. Thevenin's theorem can be applied while analyzing a circuit with dependent sources. In this case, all independent sources are turned off and the $R_{Th}$ is calculated by applying a current source or voltage source at the open terminal of the circuit. When using a voltage source, it can be assumed to be 1V for easy calculations.
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