- #1
The I and II indicate that the line integrals are being taken along two different paths between a and b.garylau said:What is Ai Aii Bi Bii in the integral?
itphyzguy said:The notations I and II are intended to indicate two different paths from a to b, as in the attached drawing. So the difference between the integral along path I and the integral along path II is equal to the integral along path I plus the integral along path II in the other direction, which is the integral around the whole loop, which is zero.
But it sound unreasonable he gives the proof like thisin fact the equation on the left side are equal to the right sidephyzguy said:The notations I and II are intended to indicate two different paths from a to b, as in the attached drawing. So the difference between the integral along path I and the integral along path II is equal to the integral along path I plus the integral along path II in the other direction, which is the integral around the whole loop, which is zero.
(I)A=>B-(II)A=>B=(I)A=>B+(II)B=>A=0 so that (I)A=>B=(II)A=>B is what he is proving.(Hopefully you can distinguish between the actual equal signs and the equal signs that I used as part of an arrow from A to B.)garylau said:it
But it sound unreasonable he gives the proof like thisin fact the equation on the left side are equal to the right side
(1)+(11)(A->B) =(1)-(11)(B->A) ?
What is Griffith trying to doing in the equation
Charles Link said:(I)A=>B-(II)A=>B=(I)A=>B+(II)B=>A=0 so that (I)A=>B=(II)A=>B is what he is proving.(Hopefully you can distinguish between the actual equal signs and the equal signs that I used as part of an arrow from A to B.)
There is one more question i want to askCharles Link said:(I)A=>B-(II)A=>B=(I)A=>B+(II)B=>A=0 so that (I)A=>B=(II)A=>B is what he is proving.(Hopefully you can distinguish between the actual equal signs and the equal signs that I used as part of an arrow from A to B.)
Ai Aii Bi Bii is a mathematical notation used to represent the components of a vector potential. The vector potential is a vector field in three-dimensional space that is used to describe the magnetic field in classical electromagnetism.
Using Ai Aii Bi Bii notation allows for a more concise and organized representation of the vector potential. It also makes it easier to perform calculations and manipulate equations involving the vector potential.
The vector potential, represented by Ai Aii Bi Bii, is related to the magnetic field through the equation B = ∇ x A, where B is the magnetic field and A is the vector potential. This equation is known as the Biot-Savart law.
Yes, Ai Aii Bi Bii notation can be used to represent components of any vector field in three-dimensional space. However, it is most commonly used to describe the vector potential in classical electromagnetism.
Ai Aii Bi Bii notation is different in that it specifically represents the components of the vector potential. Other notations, such as Cartesian coordinates or spherical coordinates, can also be used to represent vector fields, but they may not be as efficient or organized as Ai Aii Bi Bii notation for describing the vector potential.