130CHAPTER 18 (b) When the steady-state has been reached, the potential difference across Cis the same as the potential difference across because there is no change in potential across . Therefore, the charge on the capacitor is 2R3R()263210.0 F33310A010 50.0 CRVR15.QCCIµ−==××Ω==∆18.51Applying Kirchhoff’s junction rule at junction agives (1) Applying Kirchhoff’s loop rule on the leftmost
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This note was uploaded on 12/09/2011 for the course PHYS 2020 taught by Professor Staff during the Fall '10 term at FIU.