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JEE Main 2021
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Animated Solution for Physics - Electromagnetic Induction: A circular coil of radius and turns is rotated about its vertical diameter with an angular speed of in a uniform horizontal magnetic field of . The maximum emf induced in the coil will be ...... . (rounded off to the nearest integer.)

Enter Numerical Value:

Visualized Solution

\text{Faraday's Law & Motional EMF}

The Sigma Insight: Faraday's Laws of Electromagnetic Induction

Solution Diagram
Imagine you are standing in a laboratory, looking at a beautifully simple yet profoundly powerful setup: a circular coil of wire suspended in mid-air, spinning rapidly like a coin on a table. But this isn't just any spin; it's rotating precisely about its vertical diameter. Surrounding this spinning coil is an invisible, uniform horizontal magnetic field.
This is the exact physical reality of an Alternating Current (AC) generator. As the coil spins, the amount of magnetic field lines piercing through its surface—what we call the magnetic flux—is constantly changing. Sometimes the coil faces the field head-on, capturing maximum flux, and a split second later, it's edge-on, capturing none. This continuous, rhythmic change in flux is the heartbeat of electromagnetic induction.

The Master Equation

Faraday's Law
To understand how this spinning motion creates electricity, we must invoke one of the most elegant laws in all of physics: Faraday's Law of Electromagnetic Induction. Faraday discovered that nature abhors a change in magnetic flux, and it responds by inducing an electromotive force (EMF) to oppose that change.
Mathematically, the magnetic flux through a coil of turns, area , in a magnetic field is given by the dot product of the magnetic field vector and the area vector:
Because the coil is rotating with a constant angular velocity , the angle between the area vector and the magnetic field changes with time as . Substituting this in, we get:
Now, Faraday's Law tells us that the induced EMF is the negative rate of change of this flux:
Let's take the derivative of our flux equation with respect to time. The derivative of is . The negative signs cancel out, leaving us with a beautiful, oscillating function:
The question specifically asks for the maximum EMF induced in the coil. Looking at our equation, the sine function oscillates between and . Therefore, the maximum possible value of this EMF—the amplitude of our AC signal—is simply the coefficient in front of the sine term:
This is our master equation. It tells us that to get a massive voltage, we need a strong magnet (), a large coil (), lots of turns (), and we need to spin it incredibly fast ().

Gathering the Arsenal

Raw Substitution
Now that we have our master equation, let's gather the raw data provided in the problem. We are given: - Number of turns, - Magnetic field, - Angular speed, - Radius of the coil,
Before we plug anything in, we must be vigilant about units. Physics demands consistency. The radius is in centimeters, which is a trap! We must convert it to standard SI units (meters):
Now, we can calculate the area of the circular coil:
Let's substitute all these raw values into our maximum EMF formula without evaluating them just yet. Let's see the raw structure of the physics:

The Art of Calculation

Simplifying the Math
I know this long string of numbers might look intimidating, but let's take a breath. The art of calculation in physics is all about grouping friendly numbers together.
First, let's look at and . Multiplying them is incredibly satisfying:
Next, let's handle the area. Squaring gives us . So the area is:
Now, let's rewrite our expression with these simplified chunks:
Look at how much cleaner that is! Now, let's combine the powers of ten. We have (which is ) multiplied by . This simply leaves us with .
Multiply that by the from the magnetic field, and we get a neat :
Our massive equation has now collapsed into a very manageable product:
Multiplying by gives us . So, we are left with:

The Final Polish

Rounding to Victory
We are at the finish line. We need a numerical answer, so let's substitute the approximate value of :
The problem asks us to format our answer as something multiplied by . To do this, we shift the decimal point two places to the right:
Finally, the question demands that we round off to the nearest integer. Looking at , the decimal part is less than , so we round down.

The Way Forward

Changing the Axis
Before we close this chapter, let's do a quick thought experiment. What if the coil was rotated about a horizontal axis that was perfectly parallel to the magnetic field?
Visualize it. The coil is spinning, but its face is always parallel to the magnetic field lines. The area vector (which points straight out of the face of the coil) would always be perpendicular to the magnetic field .
Because the dot product of two perpendicular vectors is zero, the magnetic flux would be permanently zero. If the flux never changes, Faraday's Law tells us that absolutely no EMF would be induced!
This highlights a profound truth in electromagnetism: it's not just about having a magnetic field and a moving coil; the relative orientation is everything. The geometry of the setup dictates the physics.

Similar Questions

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A circular coil of radius is placed in a uniform magnetic field of with its plane perpendicular to the field initially. It is rotated at constant angular speed about an axis along the diameter of coil and perpendicular to magnetic field, so that it undergoes half of rotation in . The maximum value of emf induced (in ) in the coil will be close to the integer ......... .

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A planar loop of wire rotates in a uniform magnetic field. Initially at , the plane of the loop is perpendicular to the magnetic field. If it rotates with a period of about an axis in its plane, then the magnitude of induced emf will be maximum and minimum respectively at

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A uniform magnetic field exists in a direction perpendicular to the plane of a square loop made of a metal wire. The wire has a diameter of and a total length of . The magnetic field changes with time at a steady rate . The induced current in the loop is close to (Take, resistivity of the metal wire )

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A circular conducting coil of radius is being heated by the change of magnetic field passing perpendicular to the plane in which the coil is laid. The resistance of the coil is . The magnetic field is slowly switched off such that its magnitude changes in time as The energy dissipated by the coil before the magnetic field is switched off completely is .

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Two concentric circular coils and are placed in the xy-plane. has 500 turns and radius of 1 cm. has 200 turns and radius of 20 cm. carries a time dependent current , where is in secon(d) The emf induced in (in mV), at the instant is . The value of is ...... .

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A circular insulated copper wire loop is twisted to form two loops of area and as shown in the figure. At the point of crossing, the wires remain electrically insulated from each other. The entire loop lies in the plane (of the paper). A uniform magnetic field points into the plane of the paper. At , the loop starts rotating about the common diameter as axis with a constant angular velocity in the magnetic field. Which of the following options is/are correct?

* Multiple Correct Options
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The emf induced in the loop is proportional to the sum of the areas of the two loops.
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The rate of change of the flux is maximum when the plane of the loops is perpendicular to plane of the paper.
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