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Question

Question: The \(rms\) value of conduction current will be: (A) \(5.7\mu A\) (B) \(6.3\,\mu A\) (C) \(9.6...

The rmsrms value of conduction current will be:
(A) 5.7μA5.7\mu A
(B) 6.3μA6.3\,\mu A
(C) 9.6μA9.6\,\mu A
(D) 6.9μA6.9\,\mu A

Explanation

Solution

The rmsrms is the root means square value and it is the direct current which would create the same average power dissipation in a resistive load. Use th4 formula of the rmsrms value of the current and substitute the calculated value of the capacitive reactance in it to find the value of the rmsrms of the conduction current.

Useful formula:
(1) The formula of the rmsrms value of the current is given by
I=VXcI = \dfrac{V}{{{X_c}}}
Where II is the rmsrms value of the current, VV is the potential difference and Xc{X_c} is the capacitive reactance.
(2) The capacitance reactance is given by
Xc=1ωC{X_c} = \dfrac{1}{{\omega C}}
Where ω\omega is the angular frequency and CC is the capacitance.

Complete step by step solution:
In order to find the rmsrms value of the alternating current, take the formula of the rmsrms of the current
I=VXcI = \dfrac{V}{{{X_c}}}
Substitute the formula of the capacitive reactance in the above step,
I=V1ωCI = \dfrac{V}{{\dfrac{1}{{\omega C}}}}
By simplifying the above step, we get
I=V×ωCI = V \times \omega C
Substitute the value of the potential difference, angular frequency and the capacitance in the above step.
I=230×300×100×1012I = 230 \times 300 \times 100 \times {10^{ - 12}}
By simplifying the above step,
I=6.9×106AI = 6.9 \times {10^{ - 6}}\,A
Substituting the μm=106m\mu m = {10^{ - 6}}\,m in the above step,
I=6.9μAI = 6.9\,\mu A

Thus the option (D) is correct.

Note: The root means the square value of the sinusoidal wave is calculated by multiplying the 14.1414.14 with the value of the peak voltage of the sinusoidal wave. The average value of the alternating current cannot be found, since it is obtained as zero. Hence the rmsrms value is used to compare both alternating and the direct current and also the effective value of the alternating current.