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V ac and I ac are sinusoidal voltage and current at frequency = 2 f. The phasor e j t is the transformer. This is the ac circuit analysis method pioneered by Charles Proteus Steinmetz and others in the 1890s as a way to avoid having to nd the steady-state solution to the linear differential equation. If the LaPlace transform is used to de ne a linear network (with zero initial conditions) on the S -plane, we can replace S with j , which also results in an ac circuit with sinusoidal voltages and currents. We can also start at time = zero and wait for all of the transients to disappear, leaving only the steady-state ac response. The Appendix of this book looks into this subject brie y. These methods are today very popular and useful. If dc voltage and/or current are present, the dc and ac solutions can be superimposed. A sum or difference of two phasors creates the cosine wave or sine wave excitation I ac . These can be plugged into Eq. (8-1): j sin t = ej t e j t , 2 cos t = ej t + e j t 2 (8-2) asp.net upc-a UPC-A . NET Control - UPC-A barcode generator with free . NET ...
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