New User Special Price Expires in

Let's log you in.

Sign in with Facebook


Don't have a StudySoup account? Create one here!


Create a StudySoup account

Be part of our community, it's free to join!

Sign up with Facebook


Create your account
By creating an account you agree to StudySoup's terms and conditions and privacy policy

Already have a StudySoup account? Login here

110 Review and Capacitors

by: Matt Salway

110 Review and Capacitors EET 200

Matt Salway
Electrical Circuits II

Almost Ready


These notes were just uploaded, and will be ready to view shortly.

Purchase these notes here, or revisit this page.

Either way, we'll remind you when they're ready :)

Preview These Notes for FREE

Get a free preview of these Notes, just enter your email below.

Unlock Preview
Unlock Preview

Preview these materials now for free

Why put in your email? Get access to more of this material and other relevant free materials for your school

View Preview

About this Document

EET 110 summed up and the Capacitors chapter. Great review for the test upcoming.
Electrical Circuits II
Study Guide
review, Capacitors, formulas, Thevenin, Norton, Charge, Discharge, electric field
50 ?




Popular in Electrical Circuits II

Popular in Electrical Engineering

This 20 page Study Guide was uploaded by Matt Salway on Sunday September 20, 2015. The Study Guide belongs to EET 200 at Old Dominion University taught by Popescu in Fall 2015. Since its upload, it has received 83 views. For similar materials see Electrical Circuits II in Electrical Engineering at Old Dominion University.


Reviews for 110 Review and Capacitors


Report this Material


What is Karma?


Karma is the currency of StudySoup.

You can buy or earn more Karma at anytime and redeem it for class notes, study guides, flashcards, and more!

Date Created: 09/20/15
79Z W5l 1 Q 5272 27 39039 Q 4 1 39 39 2 3h L 5 f f A lt1 2Ln7lt 9191 Jv 7 m7 top 42 lt W C37 3 has GP P919AIIGP 19M d paqxosqe xamod 1A 1 T L 73 m uonuaAuoa Jamod Thevenin s Theorem Thevenin s Theorem all effects of any LINEAR circuit external to two reference terminals can be completely predicted from a model consisting of a single ideal voltage source in series with a single resistor I 2 ES V b g 3 O Req lt Ti evem n s erogedme only independent sources in the circuit 39 Determine de opencircuit voltage Vocacross the two reference terminals Vt VOC Deenergize all internal sources and determine the equivalent resistance as viewed from the two reference terminals Req Moire to deenergize independent sources replace all ideal independent voltage sources by short circuits replace all ideal independent current sources by open circuits TRANSIENTS IN CAPACITIVE NETWORKS THE CHARGING PHASE The factor t called the time constant of the network has the units of time as shown below using some of the basic equations introduced earlier in this text 2 on H ygg gwm w39 gw g 3 gsi 98 m a 352 ZBJ3U33 ul ram ma OH 2061 131 alna Japwg aBelloA CAPACITORS IN SERIES AND IN PARALLEL N Jle 423 l39 IK IY T V1 V2 V3 Q1 4quot 39 lt V 2 WE 7 E J IIII 39L I uni FIG 1067 Parallel capacitors FIG 1055 Series capacitors 576 Ila Cgi CZC 1Zl T it CT Ci CAPACITANCE The relationship connecting the applied voltage the charge on the plates and the capacitance level is defined by the following eqUation C farads F Q coulombs C V 7 volts V lt1 l 39 K i r THE CAPACITIVE CURRENT iC There is a very special relationship between the current of a capacitor and the voltage across it For the resistor it is defined by Ohm s law iR vRR The current through and the voltage across the resistor are related by a constant R a very simple direct linear relationship For the capacitor it is the more complex relationship defined by dvc Capacitive current is proportional to the rate of change of the voltage across the capacitor 4 of l 39 7 J t 4 L a a w it Cf 061 C rCZ l C4 1 SDBIBJ 111 p 5111 V quotwd uAgiuuum 3 Cd SPWBJ D uonannsuq JOlpEdEj SHOLDVdVD FORMULA SHEET Charging phase Discharging phase tRC t t vCt E1 e7 vct Ee E E E iCt Eett 6 Ee tt v vRt Ee39m vRt E84 j 2 39asoqd bullwan aql buynp 3A an 399 H 39 1 9mm mum P I 1 SQr I 9912913111 pgdtz3 3 U 939121ng 119mg r A 7 39 n3 Y EISVHd 9NEDHVHD 3HL 3SgtIHOVJ39N HAILDVdVD NI SiNEHSNVHJ Current Divider Rule is R1 R 10 t RO1R1 L5 0 e 3 3 Ti 1 Wig Wlth Tm WTm 153 3 53 y quot55quot R 332 R32 In general m 50 GoGlmGn Or i0t is QN qwomoosuomau DNi il IIBUBJIS PI9J amoela 3 sqwomoaj C9319 JI UHX nLI Illjf Mgsueq xn G39IEIlzl DIELLDEI IEI EIHL ENERGY STORED BY A CAPACITOR An ideal capacitor does not dissipate any of the energy supplied to it It stores the energy in the form of an electric field between the conducting surfaces A plot of the voltage current and power to a capacitor during the charging phase is shown in Fig 1075 The power curve can be obtained by finding the product of the voltage and current at selected instants of time and connecting the points obtained The energy stored is represented by the shaded area under the power curve Power pdt vc t ict W Energy WC prtdt U 1 1Q2 2 wczcvc 26 Equivalent resistance 0 Resistors in series R2 u v For the special case of two resistors in parallel R RequgaiMR2 9 m 3 m wWWmms 313132 m 5 W a xg INITIAL CONDITIONS Universal equation for the transient response of a capacitor eq 1021 W t W GulfA COM41w m aim Ig 39 vCt quotquot Vf tI 1 4 Va 5 Vi quot Va V53 5 CI It can be used for both charging and discharging phase CI When used for discharging make Vf 0V such that vct Vie UT Kirchhoff s Current Law Kirchhoff s current Law KCL algebraic sum of the currents at a node is zero 24 5 m 0 ML i2 t N I K 5 quot 1 Ifquot I N N 1 l t e Mm 3 I3 39wlw mw Mom M 1 mwwm 39 Nun 1 MMNV quotI l r M l r N x 1 Jquot 1 J 1 i1ti2t 1305 i4t i5t 0 Kirchhoff s Voltage Law Kirchhoff s voltage law KVL algebraic sum of the voltages around a closed W loop IS zero gg m m 0 171 t 2 t 173 t U1t 1720 1730 V4t 1250 0 Norton s Theorem Norton39s Theorem all effects of any LINEAR circuit external to two reference terminals can be completely predicted from a model consisting of a single ideal current source in parallel with a single resistor g M A I quotf1533 gt morienis firmware only independent sources in the circuit Assume a short circuit between the reference terminals Determine 56 the current that would flow through the short in isc Deenergize all internal sources and determine the equivalent resistance as viewed from the two reference terminals Req Jo 2121 14 Power and Energy 3 z Power rate of change of energy yaw m i 2 3 if units 1 watt W 1 joule of work performed in lsecond Energy total work Wm m 32 M units 1 joule J or 1 kWh kilowatthour b kWh number ofjoules quotum er of 3600 1000 3 Z Resistive Power mi N quotifFifi 5amp3 m ma 3 WE


Buy Material

Are you sure you want to buy this material for

50 Karma

Buy Material

BOOM! Enjoy Your Free Notes!

We've added these Notes to your profile, click here to view them now.


You're already Subscribed!

Looks like you've already subscribed to StudySoup, you won't need to purchase another subscription to get this material. To access this material simply click 'View Full Document'

Why people love StudySoup

Jim McGreen Ohio University

"Knowing I can count on the Elite Notetaker in my class allows me to focus on what the professor is saying instead of just scribbling notes the whole time and falling behind."

Kyle Maynard Purdue

"When you're taking detailed notes and trying to help everyone else out in the class, it really helps you learn and understand the I made $280 on my first study guide!"

Bentley McCaw University of Florida

"I was shooting for a perfect 4.0 GPA this semester. Having StudySoup as a study aid was critical to helping me achieve my goal...and I nailed it!"


"Their 'Elite Notetakers' are making over $1,200/month in sales by creating high quality content that helps their classmates in a time of need."

Become an Elite Notetaker and start selling your notes online!

Refund Policy


All subscriptions to StudySoup are paid in full at the time of subscribing. To change your credit card information or to cancel your subscription, go to "Edit Settings". All credit card information will be available there. If you should decide to cancel your subscription, it will continue to be valid until the next payment period, as all payments for the current period were made in advance. For special circumstances, please email


StudySoup has more than 1 million course-specific study resources to help students study smarter. If you’re having trouble finding what you’re looking for, our customer support team can help you find what you need! Feel free to contact them here:

Recurring Subscriptions: If you have canceled your recurring subscription on the day of renewal and have not downloaded any documents, you may request a refund by submitting an email to

Satisfaction Guarantee: If you’re not satisfied with your subscription, you can contact us for further help. Contact must be made within 3 business days of your subscription purchase and your refund request will be subject for review.

Please Note: Refunds can never be provided more than 30 days after the initial purchase date regardless of your activity on the site.