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A coil carrying electric current is placed in uniform magnetic field. Then: (a) torque is formed (b) emf is induced (c) both (a) and (b) are correct (d) none of the above.

Short Answer

Expert verified
(a) torque is formed.

Step by step solution

01

Understand the Concept

A coil carrying an electric current in a magnetic field can experience a torque or an induced emf depending on the scenario. To find the correct answer, distinguish between the effects of torque and emf.
02

Torque on a Current-Carrying Coil

When a coil carrying a current is placed in a magnetic field, it experiences a force due to the interaction between the magnetic field and the current in the wire. This force can create a turning effect, known as torque, on the coil. This phenomenon is the basic principle behind electric motors.
03

EMF in a Coil

EMF (electromotive force) can be induced in a coil if there is a change in the magnetic flux through the coil over time. This effect, called electromagnetic induction, follows Faraday's Law which states that the induced emf is proportional to the rate of change of magnetic flux.
04

Apply the Concepts

In this scenario, the coil is simply placed in a uniform magnetic field without any mention of changing magnetic flux. Therefore, while torque is generated due to the interaction of current and magnetic field, emf will not be induced as there is no change in magnetic flux through the coil.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Electromagnetic Induction
Electromagnetic induction is a fascinating concept that involves producing electric voltage (or EMF) from a changing magnetic field. Imagine a coil of wire in a magnetic environment. If you move the magnet closer or farther away, or if the coil itself moves within the magnetic field, the magnetic flux through the coil alters. This change is what induces an electromotive force (emf) in the coil, leading to an electric current if the coil is part of a closed circuit. This surprising phenomenon forms the basis for many modern technologies, like transformers and electric generators.
When we talk about changing magnetic flux, we mean how much magnetic field passes through the coil. The faster you change the magnetic environment, the stronger the induced emf. So if you want more voltage, simply increase the change—more speed or stronger magnets will do the trick.
To illustrate, think about waving a magnet quickly through a loop of wire. The quicker you wave, the more significant the electromagnetic induction, producing higher emf and current.
Faraday's Law
Faraday's Law is a key principle that helps us understand electromagnetic induction thoroughly. Formulated by Michael Faraday, this law states that the induced emf in any closed circuit is equal to the negative rate of change of the magnetic flux through the circuit. In simpler terms, if you change the magnetic field inside a loop, you create electricity.
Mathematically, Faraday's Law can be expressed as:
\[\text{emf} = - \frac{d\Phi_B}{dt}\]
where \( \Phi_B \) is the magnetic flux, which depends on the magnetic field \( B \), the area of the loop \( A \), and the angle \( \theta \) between the magnetic field and the normal to the loop.
Here are some important takeaways from Faraday's Law:
  • The minus sign in the equation signifies Lenz's law—indicating that the direction of induced emf opposes the change in flux, maintaining a balance in the system.
  • The greater the rate of change of flux, the larger the induced emf. If the change occurs slowly, the induced emf is minimal.
Faraday's Law is integral to understanding how transformers work, as they rely on changing magnetic fields within coils to transfer voltage from one circuit to another.
Electric Current in Magnetic Fields
An electric current in magnetic fields can experience unique behaviors, one of which is generating torque. This concept is central to many devices—such as electric motors—where the interaction between magnetic fields and electric currents results in mechanical motion.
When a wire carrying a current is placed in a magnetic field, it feels a force. This force comes from the magnetic field interacting with the electric current inside the wire—a result of the Lorentz force law. Torque, in this context, is the rotational equivalent of linear force. If you place a loop of wire in a magnetic field, the forces on opposite sides of the loop create a twisting action, or torque, causing the loop to spin.
Factors affecting the torque on a current-carrying loop include:
  • The magnitude of the current through the coil.
  • The strength of the magnetic field.
  • The number of turns in the coil—a coil with more loops will experience more torque.
  • The orientation of the coil relative to the magnetic field.
Understanding electric current behavior in magnetic fields is vital for controlling the motors that power countless applications, from cars to household appliances.

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Most popular questions from this chapter

A charged particle of mass \(m\) and charge \(q\) in a uniform magnetic field \(B\) acts into the plane. The plane is frictional having coefficient of friction \(\mu\). The speed of charged particle just before entering into the region is \(v_{0}\). The radius of curvature of the path after the time \(\frac{v_{0}}{2 \mu g}\) is : (a) \(\frac{m v_{0}}{q B}\) (b) \(\frac{m v_{0}}{2 q B}\) (c) \(\frac{m v_{0}}{4 q B}\) (d) none of these

The dimensions of \(\frac{1}{\sqrt{\mu_{0} \varepsilon_{0}}}\) are same as : (a) \(\frac{E}{B}\) (b) \(\frac{B}{E}\) (c) \(\frac{E^{2}}{B^{2}}\) (d) \(\sqrt{\left(\frac{E}{B}\right)}\)

The ratio of the energy required to set-up in a cube of side \(10 \mathrm{~cm}\) in a uniform magnetic field of \(4 \mathrm{~Wb} / \mathrm{m}^{2}\) and a uniform electric field of of \(10^{6} \mathrm{~V} / \mathrm{m}\), is: (a) \(1.44 \times 10^{7}\) (b) \(1.44 \times 10^{-5}\) (c) \(1.44 \times 10^{6}\) (d) \(1.44 \times 10^{3}\)

A particle of mass \(m\), carrying a charge \(q\) is lying at the origin in a uniform magnetic field directed along \(x\) -axis. At the instant \(t=0\) it is given a velocity \(v_{0}\) at an angle \(\theta\) with the \(y\) -axis, in the \(x-y\) plane. The coordinates of the particle after one revolution will be : (a) \(\left(0,0 \cdot \frac{2 \pi m v_{0} \sin \theta}{q B}\right)\) (b) \(\left(\frac{2 \pi m v_{0} \sin \theta}{q B} \cdot 0,0\right)\) (c) \(\left(\frac{2 \pi m v_{0} \sin \theta}{a B} 0,4\right)\) (d) \((0,0,0)\)

Two protons are moving with same velocity in magnetic field of same magnitude, then : (a) magnetic force on protons may be zero (b) magnetic force on both must be same to each other (c) magnetic force on both may or may not be same to each other (d) both (a) and (c) are correct

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