In many practical applications, we use variable electric current I(t), that is, the current that changes with time t. A

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In Many Practical Applications We Use Variable Electric Current I T That Is The Current That Changes With Time T A 1 (104.14 KiB) Viewed 40 times

In many practical applications, we use variable electric current I(t), that is, the current that changes with time t. A couple of examples that we will consider in this problem: (a) Current I(t)=I0​cos(2πf⋅t) that oscillates with frequency f. (b) Current I(t)=I0​e−t/τ that decays in time with time constant τ. Our questions will be related to the currents with amplitude I0​=1.59 A running in the copper (resistivity ρ=1.7×10−8Ω⋅m ) wire of diameter d=1.74 mm and length l=0.464 m. For example (a), how much energy Wa​ is dissipated in the wire via Joule heating during one period of current oscillations for frequency f=50.6 Hz? Wa​=□mJ. With the oscillating current, the amount of charge passing through any cross-section of the wire would, of course, also oscillate with the same frequency What is the amplitude Q0​ of charge oscillations?: Q0​=mC.  For example (b), how much energy Wb​ is dissipated in the wire via Joule heating during the full decay of the current (from t=0 to t=∞ ) for time constan τ=24.51 ms ?: Wb​=mJ. How much charge Qb​ passes through any cross-section of the wire during the full decay of the current?: Qb​=mC.