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de" or "blocks de" Capacitors are often utili zed to re move o r tilter out a n un wanted de vo ltage In analyz ing a c ircuit containing de volt age sources and capacitors, we can replace the capacitors wi th an open circuit and calc ulate vo ltages and c urrents in the c ircuit using o ur many analysis tools Note that the powe r absorbed by a capacito r, given by Eq (65), is directl y proportio nal to the time rate of change of the voltage across th e capacitor Wh at if we had an instamaneo us change in the capacitor vo ltage This wo ul d co rrespond to dvl d! = 00 and infinite power Bac k in I, we ruled out the possibil ity of any sources of infi nite power.

(4.15)

There is one notable difference between the program skeleton for SketchBerry and the structure for HelloBlackBerry. In HelloBlackBerry, the MainScreen class lived in the code as a separate standalone class. In SketchBerry, the SketchBerryScreen class is inside of the SketchBerry application class. Why the change Well, strictly speaking you don t have to do it this way, but making the screen class be part of the application class is an easy technique for allowing the two classes to share access to the same program data in the form of data variables. The need for each of these classes to access each other s data will become apparent in a little bit, so for now, just bear with me. So far, all you have is a general application skeleton. Now it s time to start doing some more interesting things with SketchBerry.

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Since we only have fi ni te power sources, the voltage across a capacitor cannot change instantaneously Thi s will be a particul arl y helpful idea in the nex t chapter whe n we encounter ci rcuit s containing sw itches Thi s idea of "continuity of vo ltage" fo r a capaci to r te lls us that the voltage across the capacito r just aft er a switch moves is the sa me as the vo ltage across the capac ito r just be fore th at sw itch moves The polarity of the voltage ac ross a capac itor being charged is shown in Fig 6 1b In the ideal case, the capac ito r will hold the charge fo r an inde finite peri od of time , if the so urce is removed If at so me later time an energy-absorbing device (e g .

96 100 104 108

where sm and dm are the conductivity and skin depth of aluminum, respectively. The ground-plane contribution to Rm can be ignored because the current densities in it are much smaller than those in the center conductor. The resistance RL is inserted in the equivalent circuit of Fig. 1.11.2 to account for the loss caused by the longitudinal current owing in the N semiconductor parallel to the current in the center conductor. Since the longitudinal semiconductor current ows in addition to the longitudinal current in the metal, a parallel connection has been used. The value of RL is given by 1 s S dS S

(6:22)

, a fl ash bulb) is connected across the capacito r, a di scharge current will fl ow fro m the capaci tor and , therefore, the capacitor will supply its stored e nergy to the device ..

*Mark Granovetter, The Strength of Weak Ties , American Journal of Sociology, Vol. 78, Issue 6 (1974), available at http://www.stanford.edu/dept/soc/people/faculty/granovetter/ documents/TheStrengthofWeakTies.pdf.

Appendix E. Summary of Stability Conditions We summarize the stability conditions of the learning rule dW = F(y) W, dt where o -diagonal entries of the matrix F are expressed as fij = fi (yi ) y(i ), i = j, (E.2) (E.1)

6.8 Summary

Case 4 is shown in Fig. 10. 11 f. The voltage equations in thi s case will be the same as those in case 3 except that the signs of the mutual terms will be negative. Therefore,

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