hholzer
- 36
- 0
Given the two vector fields:
<br /> \vec E and \vec B<br />
Where the first is the electric vector field
and the second is the magnetic vector field, we
have the following identity:
<br /> curl(\vec E) = -\frac{\partial \vec B } { \partial t }<br />
and further that:
<br /> curl(curl(\vec E)) = curl(-\frac{\partial \vec B } { \partial t }) <br /> = -\frac{\partial curl(\vec B) } {\partial t }<br />
I tried to prove these by defining the vector fields:
<br /> \vec E = C\frac{ \mathbf e_r } {p^2}<br />
and
<br /> \vec B = <0, 0, B><br />
where C and B are constants. But I ended up with
zero for curl(E), which cannot be right. So my reasoning
is in error somewhere.
Any insight appreciated.
<br /> \vec E and \vec B<br />
Where the first is the electric vector field
and the second is the magnetic vector field, we
have the following identity:
<br /> curl(\vec E) = -\frac{\partial \vec B } { \partial t }<br />
and further that:
<br /> curl(curl(\vec E)) = curl(-\frac{\partial \vec B } { \partial t }) <br /> = -\frac{\partial curl(\vec B) } {\partial t }<br />
I tried to prove these by defining the vector fields:
<br /> \vec E = C\frac{ \mathbf e_r } {p^2}<br />
and
<br /> \vec B = <0, 0, B><br />
where C and B are constants. But I ended up with
zero for curl(E), which cannot be right. So my reasoning
is in error somewhere.
Any insight appreciated.