Phasor

−Here,$V=Vaejθ=Va(cos⁡θ+jsin⁡θ)=Va∠θ$isthephasor−Byconvention,weusetherealpart(butdropthe$ℜ$)−Thisisusefulbecauseifwehaveasourceat$ω$frequency,allcircuitcomponentswillrunat$ω$frequency,sothere′snopointofkeepingitaround−[[F0−Glossary/ConcreteConcepts/Kirchhoff′sLaws∥Kirchhoff′sLaws]]holdherestill