Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 29 - Molecules and Solids - Problems - Page 855: 31

Answer

a) $5.14\;\rm mA$ b) $3.64\;\rm mA$

Work Step by Step

a) We know that the period of the rectified voltage is given by $$T=\dfrac{1}{f}=\dfrac{1}{120}=\bf8.33\times10^{-3}\;\rm s$$ and the time constant of this circuit is given by $$\tau=RC=(33\times 10^3)(28\times 10^{-6})=\bf0.924\;\rm s$$ Now it is obvious that the time circuit $\tau$ is much greater than the period time $\tau\gt \gt T$. This means that the voltage across the capacitor is constant during the cycle. Thus, the average voltage is equal to the maximum voltage. $$I_{avg}=\dfrac{V_{max}}{R} $$ we know that the maximum voltage is given by $$V_{max}=\sqrt{2}v_{\rm rms} $$ So, $$I_{avg}=\dfrac{\sqrt{2}v_{\rm rms}}{R} $$ Plugging the known; $$I_{avg}=\dfrac{\sqrt{2}\times 120}{33\times 10^3} $$ $$I_{avg}= \color{red}{\bf 5.14\times10^{-3}}\;\rm A$$ ________________________________ b) Now we need to find the time constant of this circuit with the new capacitor. $$\tau=RC=(33\times 10^3)(0.1\times 10^{-6})=\bf 3.3\times10^{-3}\;\rm s$$ In this case, the periodic time is greater than the time circuit $T\gt \tau$ by 2.5 times. This means that the voltage goes up and down until it reaches zero voltage. Therefore, the average voltage here is equal to the RMS voltage. $$I_{avg}=\dfrac{V_{\rm rms}}{R} =\dfrac{120}{33\times10^3}$$ $$I_{avg}= \color{red}{\bf 3.64\times10^{-3}}\;\rm A$$
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