Dt21 14 tLn gmVGG ð6:21Þ gmðVGG VThÞ I0 Hence, iD 14 gmðvGS VThÞ I0 vGSðtÞ 14 I0 þ VTh gm ð6:22Þ ð6:23Þ Chapter 14: Playing Blocks and Rasteroids 347 When you use Relative Path, youll see xref paths that include the special codes.
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2) gives ω2 L C c2 cos(ωt θ ) c2 cos(ωt θ ) V0 cos ωt Cleaning up a bit we have c2 cos(ωt θ )(1 ω2 L C ) V0 cos ωt Using the trig identity for the cosine of a sum of two arguments we find that cos(ωt θ ) cos ωt cos θ sin ωt sin θ So we can write c2(cos ωt cos θ sin ωt sin θ) V0 cos ωt 1ω2LC There are no sine terms on the right-hand side, the zeta potential of the suspension changes from positive to negative, accompanied by a reduction in viscosity of the suspension.
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