32_Chapter 18 HomeworkCH18 Direct-Current Circuits

32_Chapter 18 HomeworkCH18 Direct-Current Circuits - 130...

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130 CHAPTER 18 (b) When the steady-state has been reached, the potential difference across C is the same as the potential difference across because there is no change in potential across . Therefore, the charge on the capacitor is 2 R 3 R () 2 63 2 10.0 F 333 10 A 0 10 50.0 C R V R 15. QC CI µ == × × = =∆ 18.51 Applying Kirchhoff’s junction rule at junction a gives (1) Applying Kirchhoff’s loop rule on the leftmost
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This document was uploaded on 10/20/2011.

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