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Question: An alternating current is given by \(I = {I_1}\cos \omega t + {I_2}\sin \omega t\) . The \(RMS\) val...

An alternating current is given by I=I1cosωt+I2sinωtI = {I_1}\cos \omega t + {I_2}\sin \omega t . The RMSRMS value of current is given by:
A) I1+I22\dfrac{{{I_1} + {I_2}}}{{\sqrt 2 }}
B) (I1+I2)22\dfrac{{{{\left( {{I_1} + {I_2}} \right)}^2}}}{2}
C) I12+I222\sqrt {\dfrac{{{I_1}^2 + {I_2}^2}}{2}}
D) I12+I222\dfrac{{\sqrt {{I_1}^2 + {I_2}^2} }}{2}

Explanation

Solution

The average value of the alternating current always tends to zero. Hence the root means square value is used. From the given alternating current, square its value. Taking the square root of the mean value provides the value of the root means square of the alternating current.

Formula used:
(1) The formula of the root means square value of the current is given by
Irms=I2{I_{rms}} = \sqrt {{I^2}}
Where Irms{I_{rms}} is the root means square value of the current and II is the mean value of the current.
(2) The algebraic formula is given by
(a+b)2=a2+b2+2ab{\left( {a + b} \right)^2} = {a^2} + {b^2} + 2ab
(3) The trigonometric formula is given by
sin2θ=2sinθcosθ\sin 2\theta = 2\sin \theta \cos \theta

Complete step by step solution:
It is given that the alternating current, I=I1cosωt+I2sinωtI = {I_1}\cos \omega t + {I_2}\sin \omega t
For getting the mean value of the current, square the given alternating current,
I2=(I1cosωt+I2sinωt)2\Rightarrow {I^2} = {\left( {{I_1}\cos \omega t + {I_2}\sin \omega t} \right)^2}
By using the formula of the (a+b)2=a2+b2+2ab{\left( {a + b} \right)^2} = {a^2} + {b^2} + 2ab , we get
I2=I12cos2ωt+I22sin2ωt+2I1I2cosωtsinωt\Rightarrow {I^2} = I_1^2{\cos ^2}\omega t + {I_2}^2{\sin ^2}\omega t + 2{I_1}{I_2}\cos \omega t\sin \omega t
Since the instantaneous value of the alternating current is 45{45^ \circ } , substitute this value in the above equation, we get
I2=I122+I222+2I1I2sin2ωt\Rightarrow {I^2} = \dfrac{{I_1^2}}{2} + \dfrac{{{I_2}^2}}{2} + 2{I_1}{I_2}\sin 2\omega t
By simplifying the above step, we get
I2=I122+I222+2I1I2×0\Rightarrow {I^2} = \dfrac{{I_1^2}}{2} + \dfrac{{{I_2}^2}}{2} + 2{I_1}{I_2} \times 0
By further simplification,
I2=I122+I222\Rightarrow {I^2} = \dfrac{{{I_1}^2}}{2} + \dfrac{{{I_2}^2}}{2}
I2=I12+I222\Rightarrow {I^2} = \dfrac{{{I_1}^2 + {I_2}^2}}{2}
By taking the square root on both sides, in order to neglect the square in the left hand side of the equation.
I=I12+I222\Rightarrow I = \sqrt {\dfrac{{{I_1}^2 + {I_2}^2}}{2}}
The value of the root means the square value of the current is obtained as I=I12+I222I = \sqrt {\dfrac{{{I_1}^2 + {I_2}^2}}{2}} .

Thus the option (C) is correct.

Note: In the above solution, sinωt\sin \omega t and the cosωt\cos \omega t is substituted as the 12\dfrac{1}{{\sqrt 2 }} . Also remember the formula, sin2θ=2sinθcosθ\sin 2\theta = 2\sin \theta \cos \theta . From the above formula, it is framed as cosθsinθ=2sin2θ\cos \theta \sin \theta = 2\sin 2\theta . The root means the square value of the sinusoidal wave will produce the same heating effect similar to that of direct current.