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4.8╬й
4╬й
8.4╬й
40╬й
8╬й
To determine the impedance of the coil, we first calculate the induced electromotive force (EMF) using Faraday's Law of Electromagnetic Induction, which states that the induced EMF is the negative rate of change of magnetic flux (e=тИТdtd╧ХтАЛ). Since the resistance of the coil is R=ieтАЛ, we calculate the magnitude of the EMF at t=2 seconds and divide by the given current i=5┬аA.
To determine the impedance of the coil, we first calculate the induced electromotive force (EMF) using Faraday's Law of Electromagnetic Induction, which states that the induced EMF is the negative rate of change of magnetic flux (e=тИТdtd╧ХтАЛ). Since the resistance of the coil is R=ieтАЛ, we calculate the magnitude of the EMF at t=2 seconds and divide by the given current i=5┬аA.
e=dtd╧ХтАЛ тАФ Induced EMF from magnetic flux
Z=ieтАЛ тАФ Impedance derived from Ohm's law
According to Faraday's Law, the induced EMF magnitude is тИгeтИг=тИгdtd╧ХтАЛтИг. Given ╧Х(t)=5t2+4t+10, the derivative is dtd╧ХтАЛ=10t+4. At t=2┬аs, тИгeтИг=10(2)+4=24┬аV. Using Ohm's Law, the impedance (in this case, resistance as the circuit is treated as purely resistive) is Z=ieтАЛ=5┬аA24┬аVтАЛ=4.8┬а╬й.
Faraday's Law relates magnetic flux variation to induced EMF.
The impedance Z for a purely inductive or resistive coil at a specific instant is calculated using instantaneous values of voltage and current.
The constant term in the flux equation (10┬аWb) becomes zero upon differentiation.
Simple application of calculus to solve electromagnetic problems.
Direct calculation based on given time-dependent parameters.
Assumes the coil behavior is linear and that instantaneous impedance equals DC resistance at the given frequency/time.
Requires knowledge of derivatives.
Design of electromagnetic sensors.
Analysis of transient response in R-L circuits.
The derivative of ╧Х=5t2+4t+10 with respect to time is 10t+4.
At t=2, e=24┬аV.
Given i=5┬аA, R=524тАЛ=4.8┬а╬й.
A is correct тАФ The calculated impedance based on induced EMF and current is 4.8┬а╬й.
Always remember that in problems involving time-varying magnetic flux, the derivative represents the instantaneous EMF; never forget to differentiate the constant term, which disappears.