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the current by differentiating the voltage: dv(t) 5 6 6 = 10 7 6 e t/10 A t 0 = 05e t/10 dt 10 A plot of the capacitor current is shown in Figure 44 Note how the current jumps to 05 A instantaneously as the voltage rises exponentially: The ability of a capacitor s current to change instantaneously is an important property of capacitors iC (t) = C

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maximum charge-storage capability for that voltage (since Q = CV ) and no more current ows through the capacitor The total charge stored is Q = 05 10 6 C This is a fairly small amount of charge, but it can produce a substantial amount of current for a brief period of time For example, the fully charged capacitor could provide 100 mA of current

interplanar distance In the bcc structure, these are the {110} planes, and in the fcc structure, these are the {111} planes (Figures 222 and 223)

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It has been found possible to arrange six sex-linked factors in Drosophila in a linear series, using the number of crossovers per one hundred cases as an index of the distance between any two factors. This scheme gives consistent results, in the main. A source of error in predicting the strength of association between untried factors is found in double crossing over. The occurrence of this phenomenon is demonstrated, and it is shown not to occur as often as would be expected from a purely mathematical point of view, but the conditions governing its frequency are as yet not worked out.

There are many useful applications of this energy-storage property of capacitors in practical circuits

Known Quantities: Capacitor current; initial capacitor voltage; capacitance value Find: Capacitor voltage Schematics, Diagrams, Circuits, and Given Data:

These results . . . form a new argument in favor of the chromosome view of inheritance, since they strongly indicate that the factors investigated are arranged in a linear series, at least mathematically.

iC (t) =

Alfred H. Sturtevant (1891 1970).

vC (t = 0) = 2 V; C = 1,000 F The capacitor current is plotted in Figure 45(a)

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Fig 223: Interplanar spacing of {111} planes in (a) bcc and (b) fcc structures [26, 27]

(Courtesy of the Archives, California Institute of Technology.)

10 9 8 7 6 5 4 3 2 1 0 02

02 04 06 08 Time (s) (a)

(0.0 1.5)

12 11 10 9 8 7 6 5 4 3 2 02

A diamond can be cleaved along any plane parallel to the 111 plane or an octahedral plane (Figure 224) It behaves as if it consists of an infinite number of very thin laminations which can be

v 30.7

02 04 06 08 Time (s) (b)

Assumptions: The capacitor is initially charged such that vC (t = t0 = 0) = 2 V Analysis: Using the de ning integral relationship for the capacitor, we may obtain the

(33.0)

iC (t ) dt +vC (t0 )

further but remains now at the maximum value it reached at t = 1 s: vC (t = 1) = 12 V The nal value of the capacitor voltage after the current source has stopped charging the capacitor depends on two factors: (1) the initial value of the capacitor voltage, and (2) the history of the capacitor current Figure 45(a) and (b) depicts the two waveforms

m 33.7

Fig 224: The cleavable planes of a diamond [25]

Physical capacitors are rarely constructed of two parallel plates separated by air, because this con guration yields very low values of capacitance, unless one is willing to tolerate very large plate areas In order to increase the capacitance (ie, the ability to store energy), physical capacitors are often made of tightly rolled sheets of metal lm, with a dielectric (paper or Mylar) sandwiched in between Table 41 illustrates typical values, materials, maximum voltage ratings, and useful frequency ranges for various types of capacitors The voltage rating is particularly important, because any insulator will break down if a suf ciently high voltage is applied across it Energy Storage in Capacitors You may recall that the capacitor was described earlier in this section as an energystorage element An expression for the energy stored in the capacitor, WC (t), may be derived easily if we recall that energy is the integral of power, and that the

(36.1)

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