Magnetic Flux Φ and Moving Bar ζ: Investigating the Change

In summary, the bar of length ζ moving to the right with speed v in a uniform magnetic field B going out the page causes a differential change in flux given by dΦ=B⋅dA.
  • #1
ZARATHUSTRA
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consider the graph below, the bar of length ζ moving to the right with speed v in a uniform magnetic field B going out the page.
2ed001a8-0915-4e5d-a0c0-cbb8fc0d8ca8.gif


i don't understand why does the textbook say that there is a change in the magnetic fluxΦ? i think the area doesn't change, although it's moving. the original saying is that: During a time interval dt, the area of the loop increases by a differential rectangular strip of area dA=ldt this change in area causes a differential change in flux given by dΦ=B⋅dA ....
 
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  • #2
ZARATHUSTRA said:
i think the area doesn't change, although it's moving.
Only the blue bar is moving. The resistor is at rest. A is the area between the resistor and the bar.
 
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  • #3
TSny said:
Only the blue bar is moving. The resistor is at rest. A is the area between the resistor and the bar.
right, so... what does that mean?
 
  • #4
is it true that the moving object in motional emf has to be a conductor?
 
  • #5
and the emf created is from the separation of charges, therefore creating a potiential difference?
 
  • #6
i feel sorry to ask those stupid questions. i don't have a teacher currently teaching me AP Physics.
 
  • #7
ZARATHUSTRA said:
right, so... what does that mean?
As shown in the figure below, as the rod travels to the right the shaded area A increases. So, the amount of magnetic flux through the circuit also increases.
 

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  • #8
interesting! let me think hard about it, and thank you for your help:smile:
TSny said:
As shown in the figure below, as the rod travels to the right the shaded area A increases. So, the amount of magnetic flux through the circuit also increases.
 
  • #9
You can also look at his from a different perspective. Starting with the Lorentz force F = qv x B you can determine that the emf across the moving bar is Blv. This view is "flux cutting" of a B field (uniform or not) by a bar of length l moving with veloc ity v.

In some cases, using Faraday's law, as you did with emf = -dφ/dt, in moving media does not work. So the "Blv" law is preferred whenever media (like your bar) is moving.
ZARATHUSTRA said:
is it true that the moving object in motional emf has to be a conductor?
Yes, but not a perfect conductor. In fact, anything other than a perfect insulator.
 
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  • #10
rude man said:
You can also look at his from a different perspective. Starting with the Lorentz force F = qv x B you can determine that the emf across the moving bar is Blv. This view is "flux cutting" of a B field (uniform or not) by a bar of length l moving with veloc ity v.

In some cases, using Faraday's law, as you did with emf = -dφ/dt, in moving media does not work. So the "Blv" law is preferred whenever media (like your bar) is moving.

Yes, but not a perfect conductor. In fact, anything other than a perfect insulator.
right, i found out that there are many ways to analyse motional emf, for example, relativity, parallel capacitor, potential difference or magnetic flux, etc
 
  • #11
but the results is the same,this Blv expression occurred in a lot of the results, am i right?
 
  • #12
ZARATHUSTRA said:
and the emf created is from the separation of charges, therefore creating a potential difference?
Right.
ZARATHUSTRA said:
but the results is the same,this Blv expression occurred in a lot of the results, am i right?
Truth to tell, I'm not sure what to make of your comment. Bit of a jumble, seems like.
I restricted my comment to the generation and determination of emf by magnetic means.
 
  • #13
thanks for the reply, i found it hard to understand the magnetic field and therefore don't like to use magnetic means, too.
 

Related to Magnetic Flux Φ and Moving Bar ζ: Investigating the Change

1. What is magnetic flux Φ?

Magnetic flux Φ is a measure of the amount of magnetic field passing through a given area. It is represented in units of webers (Wb) and is calculated by multiplying the magnetic field strength by the area perpendicular to the field.

2. How is magnetic flux Φ affected by a moving bar ζ?

When a moving bar ζ is placed in a magnetic field, the magnetic flux passing through the area perpendicular to the field changes. This change in magnetic flux is directly proportional to the speed of the bar ζ and the strength of the magnetic field.

3. What is the equation for calculating the change in magnetic flux Φ?

The equation for calculating the change in magnetic flux Φ is: ΔΦ = BζΔA, where B is the magnetic field strength, ζ is the speed of the moving bar, and ΔA is the change in area perpendicular to the field.

4. How can magnetic flux Φ and the movement of bar ζ be used to investigate changes in a system?

By measuring the change in magnetic flux Φ caused by the movement of bar ζ, scientists can determine the effects of different variables on a system. This can provide valuable insights and data for further analysis and experimentation.

5. What are some real-world applications of studying magnetic flux Φ and moving bar ζ?

Magnetic flux Φ and moving bar ζ can be applied in many fields, including electrical engineering, physics, and materials science. They are commonly used in the design of motors, generators, and other electromagnetic devices. The study of these concepts is also important in understanding the behavior of magnetic materials and the effects of electromagnetic fields on them.

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