Step 1: For maximum power transfer to \(R\), set \(R=R_{\text{Th}}\), where \(R_{\text{Th}}\) is the Thevenin resistance seen from the terminals of \(R\). Replace the ideal \(10~\text{V}\) source by a short circuit.
Step 2: With the source shorted, the \(2~\text{k}\Omega\) and \(3~\text{k}\Omega\) resistors are in parallel between the middle node and ground, and this combination is in series with the \(1~\text{k}\Omega\) resistor to the \(R\) terminal. Hence,
\[
R_{\text{Th}} = 1~\text{k}\Omega + \left(2~\text{k}\Omega \parallel 3~\text{k}\Omega\right)
= 1 + \frac{2\times 3}{2+3}~\text{k}\Omega
= 1 + 1.2 = 2.2~\text{k}\Omega.
\]
Step 3: Therefore, \(R\) should be chosen as \(R_{\text{Th}}=2.2~\text{k}\Omega\) for maximum power dissipation.