Reverse engineering formulas for directing a plane wave

yefj
Messages
58
Reaction score
2
Homework Statement
plane wave
Relevant Equations
plane wave
Hello,There is a model which tunes a plane wave using certain expressions which resembles the spherical to cartesian coordinates.
There are two types of definitions:
propogation normal and electric field vector.
Why they put in propogation normal exactly the spherical to cartesian to represent propogation normal?
What is the link between propogation normal and E-field formulas?
Thanks.
1736620393551.png


1736620210292.png

1736620285342.png
 
Physics news on Phys.org
yefj said:
Why they put in propogation normal exactly the spherical to cartesian to represent propogation normal?
It looks like you have a spherical wave. The direction of propagation is radially out and a wavefront is a sphere of radius ##R##. This means that the direction of propagation at any point on the sphere is radially out, i.e. normal to the surface. A unit vector normal to the surface of a sphere is $$\mathbf{\hat n}=\sin\!\theta\cos\!\phi~\mathbf{\hat x} +\sin\!\theta\sin\!\phi~\mathbf{\hat y}+\cos\!\theta~\mathbf{\hat z}$$ which is the same as the radial unit vector ##\mathbf{\hat r}## along which the wave propagates.
 
how does E-field formulas were derived from the normal?
Thanks.
1736704647233.png
 
yefj said:
how does E-field formulas were derived from the normal?
Thanks.
View attachment 355731
The E-field vector is in the plane perpendicular to the normal. In that plane there is an infinity of directions that the E-field vector can have. Here you are given one of many. You can verify that this is a valid E-field by showing that ##~\mathbf E\cdot \mathbf{\hat n}=0.##

For a given normal you can get all the possible electric fields by varying angle ##\alpha## which rotates the electric field in the plane perpendicular to the normal. You can easily see how this works for specific choices of the angles.

For example, if I choose ##\theta=\dfrac{\pi}{2}## and ##\phi=0##, I get
(a)##~~\mathbf{\hat n}= \mathbf{\hat x}##,
(b)##~~\mathbf{\hat E}= \sin\!\alpha~\mathbf{\hat y}-\cos\!\alpha~\mathbf{\hat z}##
The above says that (a) the normal is along the ##x##-axis and (b) a unit vector in the direction of the electric field is in the ##yz##-plane and changes direction as ##\alpha## changes.
 
Hello Kuruman, I understand that E-field can have endless options.
What is the logic for choosing the expression for e-field?
Thanks.
 
yefj said:
Hello Kuruman, I understand that E-field can have endless options.
What is the logic for choosing the expression for e-field?
Thanks.
If you understand that the E-field has infinitely many options and that it must be perpendicular to the direction of propagation, there is no logic for choosing a particular direction as opposed to another. Pick a direction and move on with your life. That's what the person that made the simulation that you posted most probably did understanding that it is necessary to make a choice before drawing the surface, the normal and the E-field.
 
Thread 'Help with Time-Independent Perturbation Theory "Good" States Proof'
(Disclaimer: this is not a HW question. I am self-studying, and this felt like the type of question I've seen in this forum. If there is somewhere better for me to share this doubt, please let me know and I'll transfer it right away.) I am currently reviewing Chapter 7 of Introduction to QM by Griffiths. I have been stuck for an hour or so trying to understand the last paragraph of this proof (pls check the attached file). It claims that we can express Ψ_{γ}(0) as a linear combination of...
Back
Top