Does a constant electric flux produce a current?

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SUMMARY

A constant electric flux does not produce a current in a wire with a constant electric field, as demonstrated through Gauss' Law, which requires a closed surface for integration. The discussion clarifies that while the electric field E remains constant, the resulting electric flux is also constant, leading to zero current. However, in practical applications such as MOSFETs, a constant electric field can indeed result in a current, influenced by factors like the cross-sectional area and saturation velocity of charge carriers.

PREREQUISITES
  • Understanding of Gauss' Law and its application in electromagnetism
  • Familiarity with electric fields and their properties
  • Knowledge of current definition and charge flow
  • Basic principles of semiconductor physics, particularly MOSFET operation
NEXT STEPS
  • Study the implications of Gauss' Law in different geometries and electric field configurations
  • Learn about the Lorentz force and its effects on charge carriers in electric fields
  • Investigate the role of saturation velocity in semiconductor devices
  • Explore the relationship between electric field strength and current in MOSFETs
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Students and professionals in electrical engineering, physicists studying electromagnetism, and semiconductor engineers working with MOSFET technology.

eoghan
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Hi! Suppose I have a wire with a potential difference V=bx where b is a constant. Then there is an electric field which is constant: E=b through out the wire. Well, now consider this relation:
I=\frac{dq}{dt}=\frac{d}{dt}\epsilon_0\int{\vec{E}\cdot\hat{n}dS}=\epsilon_0 S \frac{dE}{dt}=0
where I used the Gauss' theorem and the fact that E is constant.
From this relation then follows that the electric current is 0! But I do have an electric current in the wire! Where am I wrong?
 
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What surface are you integrating over, what does "x" stand for? Could you explain the problem a little more so that I can help you, personally I can't see it. Thanks
 
Your Gaussian surface must be closed. The current flows in one side and out the other, which is why the integral is zero.
 
Zaphys said:
What surface are you integrating over, what does "x" stand for? Could you explain the problem a little more so that I can help you, personally I can't see it. Thanks

Let's say that the wire lies along the x axis.. then x represents a point of the wire. I integrate over a surface perpendicular to the wire in a point x with the center on the wire. But the surface is meaningless, what matters is that if E is constant in time, then its flux will be constant in time (if the surface is constant in time).

clem said:
The current flows in one side and out the other, which is why the integral is zero.
Yes, but if you define I=dq/dt then you have I=d/dt (flux(E)) which is zero. With the Gauss' theorem I don't get the net current in the surface (which is zero), but the charge.
 
Have it your way, but I thought you said "I used the Gauss' theorem".
 
eoghan said:
Let's say that the wire lies along the x axis.. then x represents a point of the wire. I integrate over a surface perpendicular to the wire in a point x with the center on the wire. But the surface is meaningless, what matters is that if E is constant in time, then its flux will be constant in time (if the surface is constant in time).


Yes, but if you define I=dq/dt then you have I=d/dt (flux(E)) which is zero. With the Gauss' theorem I don't get the net current in the surface (which is zero), but the charge.

clem is correct here, you used Gauss' Law to relate the charge to the electric field, but Gauss' law requires a closed surface and since you have a spacially constant electric field you will always have zero flux. You should instead try the Lorentz force, however, you would need knowledge of the saturation velocity of charges, otherwise the constant force over an infinite wire will create infinite current.

Still, in respect to your original question, yes, a constant flux can create current. I know that in a simple MOSFET model, we assume that there is a constant electric field between the source and drain which results in a current. The amount of current is limited by the finite cross-sectional area of the transistor, the finite length of the transistor, and the finite saturation velocity of the mobile carriers.
 

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