|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
magnetic flux quantum |
|
|
|
|
|
|
|
|
|
|
E Q U A T I O N S |
|
|
|
|
|
A times B |
|
|
|
|
|
|
1 |
|
Planck constant |
|
pi |
|
0.081303 |
|
|
|
2 |
|
Rydbergxhc in J |
|
proton ch/ mss qt |
|
-0.226519 |
|
|
|
3 |
|
|
|
|
|
|
|
|
|
4 |
|
|
|
|
|
|
|
|
|
5 |
|
|
|
|
|
|
|
|
|
6 |
|
|
|
|
|
|
|
|
|
7 |
|
|
|
|
|
|
|
|
|
8 |
|
|
|
|
|
|
|
|
|
9 |
|
|
|
|
|
|
|
|
|
10 |
|
|
|
|
|
|
|
|
|
|
|
A divided by B |
|
|
|
|
1 |
|
hc |
|
proton spec charg |
|
0.438889 |
|
|
|
2 |
|
S1 - S2 Hydrogen |
|
sphere radius rt2 |
|
0.749562 |
|
|
|
3 |
|
von Klitzing |
|
permeability magn |
|
0.749562 |
|
|
|
4 |
|
pi/36 |
|
sphere radius 1 |
|
0.749562 |
|
|
|
5 |
|
rd ed1 fc surface |
|
r(sp)d radius rt2 |
|
0.749562 |
|
|
|
6 |
|
sphere diam 1 |
|
8 pi |
|
0.749562 |
|
|
|
7 |
|
a u charge |
|
Hydrogen at infty |
|
0.764521 |
|
|
|
8 |
|
Wien freq displmt |
|
proton mass kg |
|
0.390871 |
|
|
|
9 |
|
|
|
|
|
|
|
|
|
10 |
|
|
|
|
|
|
|
|
|
11 |
|
|
|
|
|
|
|
|
|
12 |
|
|
|
|
|
|
|
|
|
13 |
|
|
|
|
|
|
|
|
|
14 |
|
|
|
|
|
|
|
|
|
15 |
|
|
|
|
|
|
|
|
|
16 |
|
|
|
|
|
|
|
|
|
17 |
|
|
|
|
|
|
|
|
|
18 |
|
|
|
|
|
|
|
|
|
19 |
|
|
|
|
|
|
|
|
|
20 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
The magnetic flux quantum Φ0 is the quantum of
magnetic flux passing |
|
|
through a superconductor.
The inverse of the flux quantum, 1/Φ0, |
|
|
is called the Josephson
constant, and is denoted KJ. It is the |
|
|
constant of proportionality of the Josephson
effect, relating the potential |
|
|
difference across a Josephson junction to
the frequency of the irradiation. |
|
|
|
|
|
highligted |
|
derivative |
|
nist |
|
|
|
|
|
|
|
|
|
|
|
copyright steve waterman january 2009 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|