According to the maximum power transfer theorem, maximum power is delivered to the load when the load resistance $R$ is equal to the Thevenin resistance of the rest of the circuit.
Looking at the circuit, the internal resistors form a combination that can be simplified to find Thevenin equivalent resistance across the terminals where $R$ is connected.
Using proper reduction and simplification of the internal network, we get $R_{\text{Thevenin}} = 2\ \Omega$.
Thus, for maximum power transfer, $R = R_{\text{Thevenin}} = 2 \ \Omega$