An alternating current is given by i = i1 sin ωt + i2 cos ωt. The r.m.s. current is given by
√ (i12 + i22)/ 2
(i1 + i2)/ √2
√ (i12 + i22)/ √2
(i1 - i2)/ √2
Given: \( i = i_1 \sin \omega t + i_2 \cos \omega t \)
Step 1: Square the expression
\( i^2 = (i_1 \sin \omega t + i_2 \cos \omega t)^2\)
\(= i_1^2 \sin^2 \omega t + i_2^2 \cos^2 \omega t + 2i_1 i_2 \sin \omega t \cos \omega t\)
Step 2: Average over one time period
The average of \( \sin^2 \omega t \) and \( \cos^2 \omega t \) over one time period is \( \frac{1}{2} \).
The average of \( \sin \omega t \cos \omega t \) over one time period is 0.
Therefore, the average of \( i^2 \) over one time period is:
\( \frac{(i_1^2 \sin^2 \omega t + i_2^2 \cos^2 \omega t + 2i_1 i_2 \sin \omega t \cos \omega t)}{2} = \frac{i_1^2 + i_2^2}{2}\)
Step 3: Take the square root
\( \text{r.m.s. current} = \sqrt{\frac{i_1^2 + i_2^2}{2}}\)
Comparing this result to the given options:
Therefore, the correct answer is: (A) \( \sqrt{\frac{i_1^2 + i_2^2}{2}} \).
The electrostatic potential is also known as the electric field potential, electric potential, or potential drop is defined as “The amount of work that is done in order to move a unit charge from a reference point to a specific point inside the field without producing an acceleration.”
SI unit of electrostatic potential - volt
Other units - statvolt
Symbol of electrostatic potential - V or φ
Dimensional formula - ML2T3I-1
The electric potential energy of the system is given by the following formula:
U = 1/(4πεº) × [q1q2/d]
Where q1 and q2 are the two charges that are separated by the distance d.