Question
(a) For circuits used for transporting electric power, a low power factor implies large power loss in transmission. Explain.
(b) Power factor can often be improved by the use of a capacitor of appropriate capacitance in the circuit. Explain.

Answer

(a) We know that $P=I V \cos \phi$ where $\cos \phi$ is the power factor. To supply a given power at a given voltage, if $\cos \phi$ is small, we have to increase current accordingly. But this will lead to large power loss $\left(I^2 R\right)$ in transmission.
(b)Suppose in a circuit, current $I$ lags the voltage by an angle $\phi$. Then power factor $\cos \phi=R / Z$.
We can improve the power factor (tending to 1) by making $Z$ tend to $R$. Let us understand, with the help of a phasor diagram (Fig. 7.15)
Image
how this can be achieved. Let us resolve $I$ into two components. $I _p$ along the applied voltage $V$ and $I _q$ perpendicular to the applied voltage. $I _q$ as you have learnt in Section 7.7, is called the wattless component since corresponding to this component of current, there is no power loss. $I _{ p }$ is known as the power component because it is in phase with the voltage and corresponds to power loss in the circuit. It's clear from this analysis that if we want to improve power factor, we must completely neutralize the lagging wattless current $I _{ q }$ by an equal leading wattless current $I _q^{\prime}$. This can be done by connecting a capacitor of appropriate value in parallel so that $I _{ q }$ and $I _{ q }^{\prime}$ cancel each other and $P$ is effectively $I_{ p } V$.

Need a full question paper?

Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.

Start Generating Free

Similar questions

The $\text{K}_\alpha$ X-rays of aluminium (Z = 13) and zinc (Z = 30) have wavelengths 887pm and 146pm respectively. Use Moseley's law $\sqrt{\text{v}}=\text{a}(\text{z-b})$ to find the wavelengths of the $\text{K}_\alpha$ X-ray of iron (Z = 26).
Two identical metal balls one at $\text{T}_1=300\text{K}$ and the other at $\text{T}_2=600\text{K}$ are kept at a distance of 1m in vacuum. Will the temperatures equalise by radiation? Will the rate of heat gained by the colder sphere be proportional to $\text{T}_2^4-\text{T}_1^4$ as may be expected from the Stefan's law?
A particle is subjected to two simple harmonic motions given by $\text{x}_1=2.0\sin(100\pi\text{t})$ and $\text{x}_2=2.0\sin\Big(120\pi\text{t}+\frac{\pi}{3}\Big)$ where x is in centimeter and t in second. Find the displacement of the particle at
  1. t = 0.0125.
  2. t = 0.025.
A long, straight wire carrying a current of 30A is placed in an external, uniform magnetic field of $4.0 \times 10^{-4}T$ parallel to the current. Find the magnitude of the resultant magnetic field at a point 2.0cm away from the wire.
  1. Find the radius of the circular orbit of a satellite moving with an angular speed equal to the angular speed of earth's rotation.
  2. If the satellite is directly above the north pole at some instant, find the time it takes to come over the equatorial plane. Mass of the earth $= 6 \times 10^{24}kg.$
Two circular coils of radii 5.0cm and 10cm carry equal currents of 21 A. The coils have 50 and 100 turns reepectively and are placed in such a way that their planes as well as the centres coincide. Find the magnitude of the magnetic field B at the common centre of the coils if the currents in the coils are (a) in the same sense (b) in the opposite sense.
Figure shows a square frame of wire having a total resistance r placed coplanarly with a long, straight wire. The wire carries a current i given by $\text{i}=\text{i}_0\sin\omega\text{t}.$ Find
  1. The flux of the magnetic field through the square frame.
  2. The emf induced in the frame.
  3. The heat developed in the frame in the time interval 0 to $\frac{20\pi}{\omega}.$
Find the capacitance of the combination shown in figure between A and B.
Consider a given sample of an ideal gas $\Big(\frac{\text{C}_\text{P}}{\text{C}_\text{V}}=\gamma\Big)$ having initial pressure $P_0$ and volume $V_0.$
  1. The gas is isothermally taken to a pressure $\frac{\text{P}_0}{2}$ and from there, adiabatically to a pressure $\frac{\text{P}_0}{4}.$ Find the final volume.
  2. The gas is brought back to its initial state. It is adiabatically taken to a pressure $\frac{\text{P}_0}{2}$ and from there, isothermally to a pressure $\frac{\text{P}_0}{4}.$ Find the final volume.
A wire ab of length l, mass m and resistance R slides on a smooth, thick pair of metallic rails joined at the bottom as shown in figure. The plane of the rails makes an angle θ with the horizontal. A vertical magnetic field B exists in the region. If the wire slides on the rails at a constant speed v, show that $\text{B}=\sqrt{\frac{\text{mgR}\sin\theta}{\text{vl}^2\cos^2\theta}}$