Question 6.5: An uncharged 0.2μF capacitor is driven by a triangular curr...

An uncharged 0.2μF capacitor is driven by a triangular current pulse. The current pulse is described by

i(t)={0,t05000t A, 0t20μs0.25000t A, 20t40μs;0,t40μsi(t)=\left\{\begin{array}{ll} 0, & t \leq 0 \\ 5000 t \text { A, } & 0 \leq t \leq 20 \mu \mathrm{s} \\ 0.2-5000 t \text { A, } & 20 \leq t \leq 40 \mu \mathrm{s} ; \\ 0, & t \geq 40 \mu \mathrm{s} \end{array}\right.

a) Derive the expressions for the capacitor voltage, power, and energy for each of the four time intervals needed to describe the current.

b) Plot i, v , p, and versus t. Align the plots as specified in the previous examples.

c) Why does a voltage remain on the capacitor after the current returns to zero?

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a) For t0t\leq 0,v,p,and w all are zero.

 

For 0t20μs0\leq t\leq 20\mu s;

 

v=5×106=0t(5000τ)dτ+0=12.5×109t2Vv=5\times 10^{6}=\int_{0}^{t}{\left(5000\tau \right) d\tau } +0=12.5\times10^{9}t^{2 } V,

 

p=vi=62.5×1012t3Wp=vi=62.5\times10^{12}t^{3 } W,

 

w=12Cv2=15.625×1012t4Jw=\frac{1}{2}Cv^{2}= 15.625 \times 10^{12}t^{4} J.

 

For 20μst40μs20\mu s\leq t\leq 40\mu s,

 

v=5×106=20μst(0.25000τ)dτ+5v=5\times 10^{6}=\int_{20\mu s}^{t}{\left(0.2-5000\tau \right) d\tau } +5.

 

(Note that 5 V is the voltage on the capacitor at the end of the preceding interval.) Then,

 

v=(106t12.5×109t210)Vv=\left(10^{6}t-12.5\times10^{9}t^{2 }-10\right) V,

 

p=vip=vi,

 

(62.5×1012t37.5×109t2+2.5×105t2)W\left(62.5\times10^{12}t^{3 }-7.5\times10^{9}t^{2 }+2.5\times10^{5}t-2\right) W,

 

w=12Cv2w=\frac{1}{2}Cv^{2},

 

=(15.625×1012t42.5×109t3+0.125×106t22t+105)J= \left(15.625 \times 10^{12}t^{4}-2.5 \times 10^{9}t^{3}+0.125 \times 10^{6}t^{2}-2t+10^{-5}\right) J.

 

For t40μst\geq 40 \mu s,

 

v=10Vv=10 V,

 

p=vi=0p=vi=0,

 

w=12Cv2=10μJw=\frac{1}{2}Cv^{2}=10 \mu J.

 

b) The excitation current and the resulting voltage, power, and energy are plotted in Fig. 6.12.

 

c) Note that the power is always positive for the duration of the current pulse, which means that energy is continuously being stored in the capacitor. When the current returns to zero, the stored energy is trapped because the ideal capacitor offers no means for dissipating energy. Thus a voltage remains on the capacitor after i returns to zero.

6.12

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