Phasor

Here,$V=Vaejθ=Va(cosθ+jsinθ)=Vaθ$isthephasorByconvention,weusetherealpart(butdropthe$$)Thisisusefulbecauseifwehaveasourceat$ω$frequency,allcircuitcomponentswillrunat$ω$frequency,sotheresnopointofkeepingitaround[[F0Glossary/ConcreteConcepts/KirchhoffsLawsKirchhoffsLaws]]holdherestill