Faraday's law of electromagnetism

In summary, there is a confusion regarding Faraday's law of electromagnetism and how it relates to the concept of motional emf. The conversation discusses a scenario where a conducting loop is tilted in a magnetic field, causing a change in flux but not cutting any flux lines. The experts in the conversation conclude that in practice, this situation is unlikely to happen and the mathematical equations can be set up to show that there is no change in flux. However, a simpler scenario is presented where changing the magnetic field strength would result in flux cutting and an induced emf. The original poster also mentions posting their own thread to address their confusion.
  • #1
Nimbus2000
2
0
I have a confusion regarding Faraday's law of electromagnetism. Consider this diagram
images (1).jpg

At this instant, the velocity of the rotor is parallel to the field lines, hence, no emf is induced in the rotor. Altetnatively, we can say that the rate of change of flux associated with the rotor is 0 at this instant, hence emf induced is 0.
Also, motional emf is given as E=BlvsinΘ and magnetic flux Φ=BAcosΘ. Now, E=BlvsinΘ=Bl(dx/dt)sinΘ=d(B*l*dx*sinΘ)/dt=d(BAcosΘ)/dt=dΦ/dt. This shows that if we use motional emf formula or the dΦ/dt formula, we arrive at the same result. But what if the conductor is not cutting any magnetic field and there is a change in flux with respect to the loop?
images (1).png

Suppose the middle limb is excited using a dc voltage. All the flux will be enclosed in the limb. Now consider the red loop on the middle limb. If the loop is tilted by some angle, flux through the loop will change since Θ changed. But the loop doesn't cut any flux since all the flux is enclosed in the limb. Will there be emf induced in the loop without cutting of flux lines?
Please help.
 
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  • #2
Nimbus2000 said:
Suppose the middle limb is excited using a dc voltage. All the flux will be enclosed in the limb.
A small amount of flux will be present outside the limb.

Say that the loop is just a little wider than the limb ( so that a tilt is possible ), and that the relative permeabilty, μr = 1000 as for the limb, the flux density just outside the limb will become 0.001*( density inside the limb ). So tilting the loop will cut a small amount of flux, and will induce a small amount of emf.

So just to be very accurate: An emf will be induced due to some flux lines being cut.

( Emf = dψ / dt , ψ = flux )
 
  • #3
But what if the conductor is not cutting any magnetic field and there is a change in flux with respect to the loop?
... ie if all the flux is enclosed within the loop ...

In practice this won't happen.
Mathematically we can set up anything - so set up the math and crunch the numbers.

Define a uniform magnetic field in rectangular coords: ##\vec B = B\hat k : -a/2 < x,y < a/2 ## but 0 everywhere else, and there is a square conducting loop with sides length b > a in the x-y plane, centered on the origin. You want to rotate the loop through angle ##\theta## about the y axis, being careful to keep in bounds: ##0 < \theta < \cos^{-1}(a/b)## (check?) so that the wire never cuts the magnetic field.

You want to know if there is a change in flux due to the component of ##\vec B## perpendicular to the area of the loop changing.
Is this what you are thinking of?

The equation you want is:
$$\Phi = \iint_S \vec B\cdot \text{d}\vec S$$

It needn't be that complicated: a simple situation is to change the magnetic field strength so ##\vec B = B(t)\hat k## and leave the loop in the x-y plane. Now what happens? Is flux cutting happening?
 
  • #4
Simon Bridge said:
... ie if all the flux is enclosed within the loop ...

In practice this won't happen.
Mathematically we can set up anything - so set up the math and crunch the numbers.

Define a uniform magnetic field in rectangular coords: ##\vec B = B\hat k : -a/2 < x,y < a/2 ## but 0 everywhere else, and there is a square conducting loop with sides length b > a in the x-y plane, centered on the origin. You want to rotate the loop through angle ##\theta## about the y axis, being careful to keep in bounds: ##0 < \theta < \cos^{-1}(a/b)## (check?) so that the wire never cuts the magnetic field.

You want to know if there is a change in flux due to the component of ##\vec B## perpendicular to the area of the loop changing.
Is this what you are thinking of?

The equation you want is:
$$\Phi = \iint_S \vec B\cdot \text{d}\vec S$$

It needn't be that complicated: a simple situation is to change the magnetic field strength so ##\vec B = B(t)\hat k## and leave the loop in the x-y plane. Now what happens? Is flux cutting happening?
Hesch said:
A small amount of flux will be present outside the limb.

Say that the loop is just a little wider than the limb ( so that a tilt is possible ), and that the relative permeabilty, μr = 1000 as for the limb, the flux density just outside the limb will become 0.001*( density inside the limb ). So tilting the loop will cut a small amount of flux, and will induce a small amount of emf.

So just to be very accurate: An emf will be induced due to some flux lines being cut.

( Emf = dψ / dt , ψ = flux )
Thank you @Hesch, @Simon Bridge for your replies. Actually, Nimbus2000 is my friend (and room-mate) and I was facing some technical problems while posting my own thread
https://www.physicsforums.com/threads/faradays-law-confusion.882312/.
So, he posted this thread and a few minutes later I posted my own. Later, I posted another thread in which I've asked the actual question in my mind. Please have a look and see if you can help.
https://www.physicsforums.com/threads/faradays-law-and-motional-emf-paradox.882572/.
 

What is Faraday's law of electromagnetism?

Faraday's law of electromagnetism is a fundamental law in physics that describes the relationship between a changing magnetic field and an induced electric field. It states that a changing magnetic field will induce an electric field, causing an electric current to flow.

Who discovered Faraday's law of electromagnetism?

Faraday's law of electromagnetism was discovered by the British scientist Michael Faraday in the early 19th century. He conducted a series of experiments to investigate the relationship between electricity and magnetism, leading to the discovery of this law.

What is the mathematical equation for Faraday's law of electromagnetism?

The mathematical equation for Faraday's law of electromagnetism is E = -dΦ/dt, where E represents the induced electromotive force (emf), dΦ represents the change in magnetic flux, and dt represents the change in time. This equation shows that the induced emf is directly proportional to the rate of change of magnetic flux.

What are some real-world applications of Faraday's law of electromagnetism?

Faraday's law of electromagnetism has numerous real-world applications, including generators, transformers, electric motors, and induction cooktops. It is also used in technologies such as MRI machines and power plants to generate electricity.

How does Faraday's law of electromagnetism relate to Lenz's law?

Lenz's law is a consequence of Faraday's law of electromagnetism. It states that the direction of the induced current will always oppose the change in magnetic flux that caused it. This is known as the law of conservation of energy, as the induced current creates a magnetic field that counteracts the original changing magnetic field.

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