To determine the reading on an AC ammeter connected to a circuit, we need to find the current \( I \) flowing through the circuit when the alternating EMF \( E \) is applied across an inductor.
The given EMF is:
\(E = 440 \sin(100\pi t)\)
The formula for current in an inductor when alternating EMF is applied is given by:
\(I = \frac{E_0}{Z}\)
where \( E_0 \) is the peak EMF and \( Z \) is the impedance of the inductor.
Since there is only an inductor in the circuit, the impedance \(Z = \omega L\), where:
From the given equation of EMF:
\(\omega = 100\pi\)
Given, the inductance \(L = \frac{\sqrt{2}}{\pi}\) H.
Therefore, the impedance:
\(Z = \omega L = 100\pi \times \frac{\sqrt{2}}{\pi} = 100\sqrt{2}\)
The peak EMF \( E_0 \) is given as 440 V.
Using the formula for current:
\(I = \frac{440}{100\sqrt{2}}\)
Calculate the current:
\(I = \frac{440}{100\sqrt{2}} = \frac{440}{141.42} \approx 3.11 \text{ A}\)
Since the ammeter measures the RMS value of the current, and for a sine wave:
\(I_{\text{rms}} = \frac{I_0}{\sqrt{2}}\)
Therefore, RMS current:
\(I_{\text{rms}} = \frac{3.11}{\sqrt{2}} = 2.2 \text{ A}\)
Thus, the reading on the AC ammeter will be 2.2 A, which matches the correct given option.
Current \(I = \frac{V}{\omega L}\)
\(I = \frac{440}{100\pi \times \frac{\sqrt{2}}{\pi}}\)
\(I = \frac{44}{10\sqrt{2}}\)
\(⇒\) \(I_{\text{rms}} = \frac{I}{\sqrt{2}}\)
\(=\frac{44}{20}\)
\(=2.2 A\)
So, the correct option is (C): 2.2 A
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
An alternating current can be defined as a current that changes its magnitude and polarity at regular intervals of time. It can also be defined as an electrical current that repeatedly changes or reverses its direction opposite to that of Direct Current or DC which always flows in a single direction as shown below.
Alternating current can be produced or generated by using devices that are known as alternators. However, alternating current can also be produced by different methods where many circuits are used. One of the most common or simple ways of generating AC is by using a basic single coil AC generator which consists of two-pole magnets and a single loop of wire having a rectangular shape.
AC is the form of current that are mostly used in different appliances. Some of the examples of alternating current include audio signal, radio signal, etc. An alternating current has a wide advantage over DC as AC is able to transmit power over large distances without great loss of energy.