ass3: Solve 9b, add sub letters, add todo
This commit is contained in:
@ -102,6 +102,7 @@ For the gradient we thus find
|
|||||||
The size of the supercurrent density has the same relation, $J_S \propto 1/r$.
|
The size of the supercurrent density has the same relation, $J_S \propto 1/r$.
|
||||||
|
|
||||||
\section{Superconducting wire}
|
\section{Superconducting wire}
|
||||||
|
\textbf{(a)}
|
||||||
The voltage $U = \SI{1.5e-5}{\volt}$ across the wire of length $\ell = \SI{.08}{\meter}$ induces a current $J_t$. % through the resistive wire with unknown resistivity $\rho$ according to Ohm's law.
|
The voltage $U = \SI{1.5e-5}{\volt}$ across the wire of length $\ell = \SI{.08}{\meter}$ induces a current $J_t$. % through the resistive wire with unknown resistivity $\rho$ according to Ohm's law.
|
||||||
Due to the presence of the magnetic field $B = \SI{5}{\tesla}$, if the vortices move with velocity $v_L$, a Lorentz force $f_L$ per vortex acts on the vortices.
|
Due to the presence of the magnetic field $B = \SI{5}{\tesla}$, if the vortices move with velocity $v_L$, a Lorentz force $f_L$ per vortex acts on the vortices.
|
||||||
This results in a power input $P_L = f_Lv_L = J_tBv_L$ per vortex.
|
This results in a power input $P_L = f_Lv_L = J_tBv_L$ per vortex.
|
||||||
@ -112,6 +113,18 @@ Equating these expressions and rewriting yields
|
|||||||
v_L = \frac{U}{B\ell} = \SI{3.75e5}{\meter\per\second}.
|
v_L = \frac{U}{B\ell} = \SI{3.75e5}{\meter\per\second}.
|
||||||
% https://www.wolframalpha.com/input?i=1.5*10%5E-5+%2F+%285*+.08%29
|
% https://www.wolframalpha.com/input?i=1.5*10%5E-5+%2F+%285*+.08%29
|
||||||
\]
|
\]
|
||||||
|
\todo{Direction?}
|
||||||
|
|
||||||
|
\textbf{(b)}
|
||||||
|
The vortices are aranged in a lattice with separation $r_{sep} = \sqrt{\frac{\Phi_0}{B}}$.
|
||||||
|
They move along the wire with velocity $v_L$ as determined above.
|
||||||
|
The expected frequency is then given by their velocity over the separation, as that is the period of the changing fields due to the vortices:
|
||||||
|
\[
|
||||||
|
f = \frac{v_L}{r_{sep}} = \frac{U}{B\ell}\sqrt{\frac{B}{\Phi_0}} = \frac{U}{\ell\sqrt{B\Phi_0}} = \SI{1.84}{\kilo\hertz},
|
||||||
|
% https://www.wolframalpha.com/input?i=1.5*10%5E-5+%2F+%28.08%29+%2Fsqrt%285+*+2.067*10%5E%28-15%29%29
|
||||||
|
\]
|
||||||
|
where we used that $\Phi_0 = \SI{2.067e-15}{\volt\second}$.
|
||||||
|
This is very close to what is written in the assignment, but not precisely the same, so maybe I used a different value for $\Phi_0$.
|
||||||
|
|
||||||
\section{Fine type-II superconducting wire}
|
\section{Fine type-II superconducting wire}
|
||||||
|
|
||||||
|
|||||||
Reference in New Issue
Block a user