Xref: utzoo sci.electronics:6409 sci.physics:8403 Path: utzoo!utgpu!jarvis.csri.toronto.edu!rutgers!ukma!tut.cis.ohio-state.edu!quanta.eng.ohio-state.edu!parts.eng.ohio-state.edu!abali From: abali@parts.eng.ohio-state.edu (Bulent Abali) Newsgroups: sci.electronics,sci.physics Subject: Re: Re^2: HV Cap Fun! Message-ID: <2329@quanta.eng.ohio-state.edu> Date: 2 Jun 89 15:49:52 GMT References: <4924@m2c.M2C.ORG> <3806@mit-amt> <20772@quacky.mips.COM> <166@mother.dde.uucp> <147@sierra.stanford.edu> Sender: news@quanta.eng.ohio-state.edu Reply-To: abali@parts.eng.ohio-state.edu (Bulent Abali) Organization: Ohio State Univ, College of Engineering Lines: 21 In article <147@sierra.stanford.edu> siegman@sierra.UUCP (Anthony E. Siegman) writes: >Put a small resistor, or a small inductance, or both, in series with >the switch; solve the circuit equations for the transient behavior >starting when the switch closes; and examine for physical >significance, considering particularly the case when the series R >or L tend to zero Exactly. A resistor R can be assumed in series with the switch, and the energy dissipated on R can be derived (easy). The resulting equation will show that the energy dissipated is R independent. One half of the original energy of the system will be lost on R, regardless of its value. If L is assumed instead of R, we can arrive at the same conclusion except that the 1/2 energy will not be lost, but will be stored in the inductor regardless of its value. -=- Bulent Abali Ohio State Univ., Dept.of Electrical Eng. 2015 Neil Av. Columbus, Ohio 43210 abali@baloo.eng.ohio-state.edu