Consider the Electric Field E(t,x,y,z) = Acos(ky-wt)k

In summary, you are trying to solve for the electric field using the curl of the magnetic field and you are not getting it. You need to integrate the curl of the magnetic field with respect to t to get the electric field.
  • #1
Smazmbazm
45
0

Homework Statement


Consider the Electric Field [itex]E(t,x,y,z) = A\cos(ky-wt)\hat{k}[/itex]

a) Find the magnetic field such that [itex]\partial_t B + \nabla \times E = 0 [/itex]
b) Show that ##\nabla \cdot E = 0## and that ##\nabla \cdot B = 0##.

The Attempt at a Solution



So for part a, the curl of [itex]E = -\partial B / \partial t [/itex]

Curl of E works out to be [itex]-Ak\sin(ky-wt)[/itex] I think but then I'm not sure how you get the magnetic field.

For part b, div E = 0. I don't understand how to get this. I do the calculations and get [itex]-A*t*\sin(k*y - t*w) - A*y*\sin(k*y - t*w)[/itex]? Where am I going wrong? I don't know how to do the second part at all, div B = 0.

Thanks in advanced
 
Last edited by a moderator:
Physics news on Phys.org
  • #2
Smazmbazm said:

Homework Statement


Consider the Electric Field [itex]E(t,x,y,z) = Acos(ky-wt)\hat{k}[/itex]

a) Find the magnetic field such that [itex]\partial t B + \nabla \times E = 0 [/itex]
b) Show that \nabla \cdot E = 0 and that \nabla \cdot B = 0.

The Attempt at a Solution



So for part a, the curl of [itex]E = -\partial B / \partial t [/itex]

Curl of E works out to be [itex]-Aksin(ky-wt)[/itex] I think but then I'm not sure how you get the magnetic field.
The curl of a vector field is a vector field. What is the direction vector?

Find B by solving the equation you are given:
[tex]\nabla\times \vec{E}= -\frac{\partial\vec{B}}{\partial t}[/tex]

For part b, div E = 0. I don't understand how to get this. I do the calculations and get [itex]-A*t*sin(k*y - t*w) - A*y*sin(k*y - t*w)[/itex]? Where am I going wrong? I don't know how to do the second part at all, div B = 0.
div fi+ gj+ hk is f_x+ g_y+ h_z. n Here f and g are 0 while h is a function only of y and t, not z.

Thanks in advanced
 
Last edited by a moderator:
  • #3
Hi Smazmbazm! :smile:

(i assume k is the unit vector in the z direction)
Smazmbazm said:
Curl of E works out to be [itex]-Aksin(ky-wt)[/itex]

in which direction? :wink:
For part b, div E = 0. I don't understand how to get this. I do the calculations and get [itex]-A*t*sin(k*y - t*w) - A*y*sin(k*y - t*w)[/itex]?

i'm not sure how you got that :confused:

div is simply ∂/∂x of the x coordinate + … + …

try again :smile:
 
  • #4
Right so for the first part [itex] \nabla \times E = [\partial / \partial y Acos(ky - wt) - 0]\hat{i} + [\partial / \partial x Acos(ky - wt) - 0]\hat{j} + [0 - 0]\hat{k} [/itex].

[itex]\nabla \times E = -Aksin(ky - wt)\hat{i}[/itex], correct?

For b, right. I think I confused myself. The definition of div is [itex]\partial f / \partial x + \partial g / \partial y + \partial h / \partial z [/itex]. Is that f, g and h referring to each direction? Like [itex]\hat{i}, \hat{j}, \hat{k}[/itex]? If so, that makes more sense

Thanks guys
 
  • #5
Smazmbazm said:
[itex]\nabla \times E = -Aksin(ky - wt)\hat{i}[/itex], correct?

correct :smile:
The definition of div is [itex]\partial f / \partial x + \partial g / \partial y + \partial h / \partial z [/itex]. Is that f, g and h referring to each direction? Like [itex]\hat{i}, \hat{j}, \hat{k}[/itex]?

yup, that's div(f,g,h) :smile:
 
  • #6
Sorry the previous post should be [itex]\partial B / \partial t = -Aksin(ky - wt)\hat{i} [/itex] rather then [itex]\
\nabla \times E = -Aksin(ky - wt)\hat{i} [/itex]

So to get the electric field you integrate -Aksin(ky - wt) with respect to t? Not sure where to go from there..
 
  • #7
Smazmbazm said:
So to get the electric field you integrate -Aksin(ky - wt) with respect to t? Not sure where to go from there..

Now I'm getting confused …

isn't it the magnetic field that you want? :confused:

Yes, integrate ∂B/∂t wrt t, and you get B. :smile:
 
  • #8
tiny-tim said:
isn't it the magnetic field that you want? :confused:

Yes, sorry, magnetic not electric. Ok, thanks tiny-tim
 

FAQ: Consider the Electric Field E(t,x,y,z) = Acos(ky-wt)k

What is the physical meaning of the electric field given by E(t,x,y,z) = Acos(ky-wt)k?

The electric field given by this equation represents a wave propagating in the y-direction with a wavelength of 2π/k and a frequency of w/2π. The amplitude of the wave is A and it is polarized along the k-direction.

How does changing the value of A affect the electric field?

Changing the value of A will change the amplitude of the electric field wave. This means that the strength of the electric field at any given point will increase or decrease depending on the value of A. A larger value of A will result in a stronger electric field.

What is the significance of the k vector in this electric field equation?

The k vector represents the direction of propagation of the wave. In this case, it is in the y-direction. The magnitude of the k vector is equal to 2π/λ, where λ is the wavelength of the wave. This vector also determines the spatial variation of the electric field.

How does the frequency of the electric field wave relate to the value of w in the equation?

The frequency of the electric field wave is equal to w/2π, where w is the angular frequency. This means that as the value of w increases, the frequency of the wave will also increase. The frequency is inversely proportional to the period of the wave, meaning that a higher frequency corresponds to a shorter period.

Can this electric field equation be used to describe real-world situations?

Yes, this electric field equation can be used to describe real-world situations. It is commonly used to describe electromagnetic radiation and can be applied to various systems and scenarios, such as radio waves, microwaves, and light waves.

Back
Top