The Thevenin voltage (Vth) is the open-circuit voltage across the output terminals
To find Vth, we remove any load and calculate the voltage at the terminals
First, consider the circuit without the 2 \(\Omega\) resistor connected to the output terminals
We need the voltage across the 6 \(\Omega\) resistor, as this is the voltage at the node before the 2 \(\Omega\) resistor
The 6 V source is connected to the 3 \(\Omega\) and 6 \(\Omega\) resistors which form a voltage divider (as they appear in series from the source's perspective when calculating the voltage across the 6 \(\Omega\) part)
Voltage across the 6 \(\Omega\) resistor (let's call this \(V_{node}\)) is:
$$ V_{node} = V_{source} \times \frac{R_{parallel}}{R_{series} + R_{parallel}} = 6 \, \text{V} \times \frac{6 \, \Omega}{3 \, \Omega + 6 \, \Omega} $$
$$ V_{node} = 6 \, \text{V} \times \frac{6}{9} = 6 \, \text{V} \times \frac{2}{3} = 4 \, \text{V} $$
Now, consider the output terminals where Vth is measured
Since the terminals are open-circuited, no current flows through the 2 \(\Omega\) resistor
Therefore, there is no voltage drop across the 2 \(\Omega\) resistor
The voltage at the output terminal is the same as the voltage at the node before the 2 \(\Omega\) resistor
$$ V_{th} = V_{node} = 4 \, \text{V} $$
The Thevenin voltage is 4 V