The Poynting vector represents the flow of energy per unit area and is applicable to both static and time-varying electromagnetic fields. The Poynting theorem, derived from Maxwell's equations, confirms its validity in all scenarios, including steady currents as illustrated in Griffiths' Example 8.1. In this example, the power flow along a wire is calculated using the voltage across the wire and the current, demonstrating the theorem's practical application. Analyzing energy flow in a DC coaxial cable further exemplifies the Poynting vector's relevance in stationary problems. This discussion emphasizes the importance of understanding energy transport in electromagnetic systems.