Note that the charge Q all came from the power supply through the resistor ) During the chargingthe power delivered by the supply is P = IV The energy delivered by the supply is powerxtime, or since l is varying during charging E=V int I dt=VQ since I is just charge per time. Compute the energy E = VQ delivered by the supply and compare with the energy of the fully-charged capacitorWhat happened to the rest of the energy? %3D

Introductory Circuit Analysis (13th Edition)
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Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
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Note that the charge Q all came from the power
supply through the resistor ) During the chargingthe
power delivered by the supply is P = IV The energy
delivered by the supply is powerxtime, or since lis
varying during charging E=V int I dt=VQ since I is just
charge per time. Compute the energy E = VQ
delivered by the supply and compare with the energy
of the fully-charged capacitorWhat happened to the
rest of the energy?
%3D
Transient RC response. Consider the following circuit with R-1 k2, C=0.1 µF and V-10
Volts. Initially the capacitor is discharged (Vc-0) and the switch is open as shown, so no
current flows. At time t-0 the switch is closed, allowing current to flow through the resistor
and charge up the capacitor.
R
Transcribed Image Text:Note that the charge Q all came from the power supply through the resistor ) During the chargingthe power delivered by the supply is P = IV The energy delivered by the supply is powerxtime, or since lis varying during charging E=V int I dt=VQ since I is just charge per time. Compute the energy E = VQ delivered by the supply and compare with the energy of the fully-charged capacitorWhat happened to the rest of the energy? %3D Transient RC response. Consider the following circuit with R-1 k2, C=0.1 µF and V-10 Volts. Initially the capacitor is discharged (Vc-0) and the switch is open as shown, so no current flows. At time t-0 the switch is closed, allowing current to flow through the resistor and charge up the capacitor. R
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