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MHT CET 202625 AprilMorning Shift
Exam
MHT CET
Year
2026
Date
25 April
Shift
Morning Shift
Subject
Physics
Chapter
Alternating Current

MHT CET 2026 · 25 April · Morning Shift · Physics · Alternating Current

An alternating current is given by i = i_1 ω t - i_2 ω t . The rms...

An alternating current is given by i=i1sin⁡ωt−i2cos⁡ωti = i_1\sin\omega t - i_2\cos\omega t. The rms current is given by

Options

  1. Ai1+i22\dfrac{i_1 + i_2}{\sqrt{2}}
  2. Bi12+i222\dfrac{\sqrt{i_1^2 + i_2^2}}{2}
  3. Ci12+i222\sqrt{\dfrac{i_1^2 + i_2^2}{2}}
  4. Di12+i22\sqrt{i_1^2 + i_2^2}

Correct answer

C. i12+i222\sqrt{\dfrac{i_1^2 + i_2^2}{2}}

Step-by-step solution

The given alternating current is i=i1sin⁡ωt−i2cos⁡ωti = i_1\sin\omega t - i_2\cos\omega t

The mean square value of the current over a complete cycle is:

<i2>=<(i1sin⁡ωt−i2cos⁡ωt)2><i^2> = <(i_1\sin\omega t - i_2\cos\omega t)^2>

<i2>=i12<sin⁡2ωt>+i22<cos⁡2ωt>−2i1i2<sin⁡ωtcos⁡ωt><i^2> = i_1^2 <\sin^2\omega t> + i_2^2 <\cos^2\omega t> - 2i_1 i_2 <\sin\omega t \cos\omega t>

Using the standard average values over a full cycle: <sin⁡2ωt>=12< \sin^2\omega t > = \dfrac{1}{2}, <cos⁡2ωt>=12< \cos^2\omega t > = \dfrac{1}{2}, and <sin⁡ωtcos⁡ωt>=0< \sin\omega t \cos\omega t > = 0

<i2>=i12(12)+i22(12)−0=i12+i222<i^2> = i_1^2 \left(\dfrac{1}{2}\right) + i_2^2 \left(\dfrac{1}{2}\right) - 0 = \dfrac{i_1^2 + i_2^2}{2}

The rms current is the square root of the mean square current:

irms=<i2>=i12+i222i_{rms} = \sqrt{<i^2>} = \sqrt{\dfrac{i_1^2 + i_2^2}{2}}

Answer: i12+i222\sqrt{\dfrac{i_1^2 + i_2^2}{2}}
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