Fairly hard induced EMF problem

EMF?In summary, the conversation discusses how to calculate the induced EMF in a circular coil with a time-varying magnetic field. The formula EMF=Acos(phi)(db/dt) is mentioned, as well as an alternative method to calculate the dot product between two vectors. The conversation also discusses the use of the angle phi, which can be represented by an expression varying with time. Finally, a link is provided for a more fundamental formula for calculating the induced EMF.
  • #1
RememberYourAngles

Homework Statement


6.gif

(ignore the suggested problems for test 3.)
If for whatever reason the image doesn't load the given's are that:
The area is 25pi(.125m)^2 (A circular coil with 25 turns and a radius of 12.5cm.) The magnetic field varies with time and is: (1.5T/s)t I hat + (3.33T-(2.25(T/s^2)t^2))J hat -(2.10T)k hat The Area lies flat on the xz plane.[/B]

Homework Equations


EMF=Acos(phi)(db/dt) (as only the magnetic field varies with time. [/B]

The Attempt at a Solution


Area has already been given.
db/dt=(1.5T/s)I hat -(4.5T/s)t J hat
The problem arises when I try to calculate phi.
My first instinct was to use phi as the angle between the normal of the area and db/dt (rather than B) but this was incorrect.
I know now that we can calculate phi with the following formula:
B dot A=BAcos(phi)
As the normal to the area lies purely in the J hat direction BxAx and BzAz are both zero.
Which leaves us with:
ByAy=BAcos(phi)
The problem is that the magnetic field we're given varies with time. How do we remove this dependency (if we even have to) to use this formula to calculate?
My first instinct is that we turn this:
(1.5T/s)t I hat + (3.33T-(2.25(T/s^2)t^2))J hat -(2.10T)k hat
Into this:
(1.5T/s)s I hat + (3.33T-(2.25(T/s^2)s^2))J hat -(2.10T)k hat
Leaving us with:
(1.5T)I hat + (1.08T)J hat -(2.10T)k hat
But I'm unsure whether or not this is actually correct.[/B]
 
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  • #2
There is another way to calculate the dot product between two vectors, which you do not need to actually know the value of the angle.
You can just multiply the components, then add them.
For example if vector u = ai + bj + ck and vector v = di + ej + fk, then the scalar product of u and v is a*d + b*e + c*f. This will work, even if the vectors are represented by expressions, rather than just numbers. Now you have a time varying expression for A dot dB. A is the vector normal to the xz plane.
 
  • #3
That's literally what I did.
Regardless we're only doing that dot product to get the angle phi.
 
  • #4
You can determine ##B_y## by examining the expression for ##\vec{B}##.

##B_y## is the coefficient of ##\hat{j}##.
 
  • #5
scottdave said:
There is another way to calculate the dot product between two vectors, which you do not need to actually know the value of the angle.
You can just multiply the components, then add them.
For example if vector u = ai + bj + ck and vector v = di + ej + fk, then the scalar product of u and v is a*d + b*e + c*f. This will work, even if the vectors are represented by expressions, rather than just numbers. Now you have a time varying expression for A dot dB. A is the vector normal to the xz plane.
Yeah there's no new information here unless I'm missing something.
What I am getting from this is that we can have the angle phi be represented by an expression varying with time rather than a concrete number:
Arccos((3.33T-(2.25(T/s^2)t^2))(25pi(.125m)^2)/sqrt((1.5T/s)t)^2 + (3.33T-(2.25(T/s^2)t^2))^2 +(2.10T)^2))(25pi(.125m)^2)
 
  • #6
Mister T said:
You can determine ##B_y## by examining the expression for ##\vec{B}##.

##B_y## is the coefficient of ##\hat{j}##.
Yes...
The coefficient being...?
Remember it varies with time and the J hat part has a part with no reliance on time, and one with a reliance.
 
  • #7
RememberYourAngles said:
Yeah there's no new information here unless I'm missing something.
What I am getting from this is that we can have the angle phi be represented by an expression varying with time rather than a concrete number:
Arccos((3.33T-(2.25(T/s^2)t^2))(25pi(.125m)^2)/sqrt((1.5T/s)t)^2 + (3.33T-(2.25(T/s^2)t^2))^2 +(2.10T)^2))(25pi(.125m)^2)
I feel like emitting a roar of triumph that a lion would find intimidating.
This means that phi also varies with time.
Which means our combined equation is:
EMF=Acos(phi)(db/dt)+BA-sin(phi)(dphi/dt)
Where A is 25pi(.125m)^2

Phi is Arccos((3.33T-(2.25(T/s^2)t^2))(25pi(.125m)^2)/sqrt((1.5T/s)t)^2 + (3.33T-(2.25(T/s^2)t^2))^2 +(2.10T)^2))(25pi(.125m)^2

db/dt (1.5T/s)I hat -(4.5T/s)t J hat

B is (1.5T/s)t I hat + (3.33T-(2.25(T/s^2)t^2))J hat -(2.10T)k

and dphi/dt is whatever the nasty lookin' derivative of
Arccos((3.33T-(2.25(T/s^2)t^2))(25pi(.125m)^2)/sqrt((1.5T/s)t)^2 + (3.33T-(2.25(T/s^2)t^2))^2 +(2.10T)^2))(25pi(.125m)^2 is
 
  • #8
Can someone see a problem with this math so long as we have a time (an actual number of seconds) to plug in?
The only thing I'm not sure of is whether or not to use the full B or the j hat part.
 
  • #9
RememberYourAngles said:
That's literally what I did.
Regardless we're only doing that dot product to get the angle phi.
So one way to find the dot product of two vectors is to find the magnitude of each vector, then multiply by the angle between them, this is what your formula
EMF=|A| cos(phi)(d|B|/dt) is doing. But you can find the dot product the way, below, which doesn't even need the cosine or the angle.

{scalar product of u and v is a*d + b*e + c*f., if vector u = ai + bj + ck and vector v = di + ej + fk }

This link talks about calculating the induced EMF, without mentioning anything about cosines.
https://webhome.phy.duke.edu/~schol/phy152/howtos/faraday_howto.pdf
Whoops, the one above, is the one that I intended. The one below is OK too, but it talks about the angle and cosines.
http://physics.bu.edu/~duffy/PY106/InducedEMF.html
 
Last edited:
  • #10
RememberYourAngles said:
EMF=Acos(phi)(db/dt)
You might find it easier to work with a more fundamental formula.
In terms of the area and field vectors and the number of turns, what is the total flux? What function of that determines the EMF?
 
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  • #11
RememberYourAngles said:
Can someone see a problem with this math so long as we have a time (an actual number of seconds) to plug in?
The only thing I'm not sure of is whether or not to use the full B or the j hat part.

Please use LaTeX to write your equations. Few if any will read them in the format you've written.
 
  • #12
If you want to use cos(φ), then I suggest you do this. Break it up into 3 different components of B and find 3 angles: φi, φj and φk.
So find the angle φi between the i component, and the vector normal to xz plane,
then find the angle φj between the j component, and the vector normal to xz plane,
and finally the angle φk between the k component, and the vector normal to xz plane. What are the cosines of each of those angles?
 
  • #13
Mister T said:
Please use LaTeX to write your equations
Or if not comfortable with Latex, at least use the superscript, subscript and Greek characters available with the buttons above the text area (X2, X2, Σ).
 
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  • #14
RememberYourAngles said:
Can someone see a problem with this math
I can see that you are making it a deal more complicated than it is. You can leave the vectors behind quite quickly and never need to find the angle.
Please try my suggestion in post #10.
 
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  • #15
Yes I agree with @haruspex . The solution to the problem can be much simpler than you are making it.
 

Related to Fairly hard induced EMF problem

1. What is "fairly hard induced EMF problem"?

The "fairly hard induced EMF problem" refers to a phenomenon in which a changing magnetic field creates an electric field, resulting in an induced electromotive force (EMF) in a conducting loop or circuit.

2. What causes the "fairly hard induced EMF problem"?

The "fairly hard induced EMF problem" is caused by Faraday's law of induction, which states that a changing magnetic field will induce an electric field and create an EMF in a conductor.

3. How does the "fairly hard induced EMF problem" affect electronics?

The "fairly hard induced EMF problem" can cause interference and damage to electronic devices due to the induced electric fields and currents. This is why electromagnetic shielding and grounding techniques are used in electronic design.

4. How can the "fairly hard induced EMF problem" be mitigated?

The "fairly hard induced EMF problem" can be mitigated by using shielding and grounding techniques, as well as by designing circuits and devices to be less susceptible to induced EMF. In addition, reducing the distance between the source of the changing magnetic field and the affected circuit can also help decrease the induced EMF.

5. Is the "fairly hard induced EMF problem" a common issue in everyday life?

The "fairly hard induced EMF problem" is a common issue in everyday life, as it is a natural phenomenon that occurs whenever there is a changing magnetic field, such as in power lines, motors, and electronic devices. However, with proper design and precautions, its effects can be minimized.

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