When is the Curl of Electric Displacement Zero?

In summary: Similarly, for cylindrical and planar symmetries, you can show that the curl of P is zero as well. In summary, the condition for the curl of electric displacement to be zero is satisfied in electrostatics when there is no polarization, uniform polarization, or when there is no free charge present. In addition, in systems with spherical, cylindrical, or plane symmetry, the curl of P is automatically zero, leading to a direct relationship between the curl of D and the system's symmetry.
  • #1
fricke
39
3
In what condition(s) curl of electric displacement is zero?

Is it okay to say curl of electric displacement is zero in:
1) in electrostatics (curl of E is zero)
then followed by the following conditions:
2) when there is no polarization (curl of P is zero)
3) in uniform polarization (which makes curl of P is zero)
4) when there is no free charge presents (directly obtain electric displacement D is zero and thus curl of D is zero)

and one more, how does zero curl of electric displacement related with the symmetry?
because in Griffith 4th edition book says:
"If the problem exhibits spherical, cylindrical, or plane symmetry, then you can get D directly from equation by the usual Gauss's law methods. (Evidently in such cases curl of P is automatically zero)"
 
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  • #2
We have ##\mathbf{D} = \epsilon_0 \mathbf{E} + \mathbf{P}##. Applying curl on both sides and requiring the curl of electric field displacement to be zero we obtain ##\epsilon_0 \nabla \times\mathbf{E} = -\nabla \times \mathbf{P}##. This is the general requirement for both electrostatic and electrodynamics for curl of D to be zero. So, point 2) and 3) are strictly for electrostatic case. In addition to point 2) and 3), consider also the case where ##\mathbf{P} = \nabla f## where ##f## is some scalar function. This last condition might be too rare to find in reality as compared to P being zero or uniform, but it still satisfy ##\nabla \times \mathbf{P} = 0##. As for point 4), what you mention there is only a special case for which there is no free charge. The point to remember is that in the Gauss equation ##\nabla \cdot \mathbf{D}(\mathbf{r}) = \rho_f (\mathbf{r})##, ##\rho_f (\mathbf{r})## is the charge density at a position ##\mathbf{r}##. Even if there is no free charge at this point, there might be another charge at other positions causing the D to be non zero. More generally, Gauss law only tells us the divergence of D, in order to completely characterize D we also need to know its curl. In other words, we can't really say anything about the curl from the divergence or vice versa, for there are certain vector fields whose divergence is zero but the curl is not.
fricke said:
"If the problem exhibits spherical, cylindrical, or plane symmetry, then you can get D directly from equation by the usual Gauss's law methods. (Evidently in such cases curl of P is automatically zero)"
For example, if the system exhibits spherical symmetry, the D field vector can only be radial, it has no angular components. Furthermore, it must be only a function of ##r##. So ##\mathbf{D} = \hat{r}D(r)##. Now compute the curl of P which is equal to the curl of D in electrostatic and you should see curl of P is zero.
 
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FAQ: When is the Curl of Electric Displacement Zero?

What is the definition of "Curl of electric displacement"?

The curl of electric displacement, also known as the curl of electric flux density, is a measure of the circulation of the electric field around a point in space. It is a vector quantity that describes the rotation of the electric field lines.

What is the mathematical expression for "Curl of electric displacement"?

The mathematical expression for the curl of electric displacement is given by the cross product of the del operator (∇) and the electric displacement vector (D). This can be written as ∇ x D.

How is "Curl of electric displacement" related to the electric field?

The curl of electric displacement is directly related to the electric field. In fact, it is equal to the negative of the time derivative of the electric field. This means that if the electric field is changing over time, the curl of electric displacement will also change.

What is the physical significance of "Curl of electric displacement"?

The curl of electric displacement has physical significance in understanding the behavior of electric fields. It helps us to determine the direction and magnitude of the electric field lines, and can also provide insight into the motion of charges in an electric field.

How is "Curl of electric displacement" used in practical applications?

The curl of electric displacement is important in a variety of practical applications, such as in the design of electronic devices, electromagnetic wave propagation, and in the study of electrical currents and circuits. It is also a key concept in Maxwell's equations, which describe the behavior of electric and magnetic fields.

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