Leak resistance across a spherical cell
Through what resistance does the charge on a sphere-in-sphere cell leak away?
- R
- Leak resistance, Ω
- a
- Inner diameter, in
- b
- Outer diameter, in
- σ
- Conductivity, µS/cm
LaTeX
R = \frac{1}{2\pi \cdot σ} \left( \frac{1}{a} - \frac{1}{b} \right)
Result
R
Leak resistance
106.9 Ω
The resistance of the water between the spheres.
LaTeX
106.9\,\mathrm{Ω} = \frac{1}{2\pi \cdot 390.6\,\mathrm{µS/cm}} \left( \frac{1}{0.5\,\mathrm{in}} - \frac{1}{0.75\,\mathrm{in}} \right)
Worth knowing
- A leak of 107 Ω is a short as far as step charging is concerned. Only distilled or deionised water gets the leak into the kilohms.
This result is a link — the address bar holds your numbers, so it can be pasted into a post and opened to the same answer.
What this looks like
The formula behind the curve
- R
- Leak resistance, Ω
- a
- Inner diameter, in
- b
- Outer diameter, in
- σ
- Conductivity, µS/cm
LaTeX
R = \frac{1}{2\pi \cdot σ} \left( \frac{1}{a} - \frac{1}{b} \right)
The formula behind the curve
- R
- Leak resistance, Ω
- a
- Inner diameter, in
- b
- Outer diameter, in
- σ
- Conductivity, µS/cm
LaTeX
R = \frac{1}{2\pi \cdot σ} \left( \frac{1}{a} - \frac{1}{b} \right)
Method
- Convert the diameters to metres and the conductivity to siemens per metre.
- The resistance between concentric spheres of radii r_a and r_b through a conductor is (1/(4πσ))(1/r_a − 1/r_b). Written in diameters the 4π becomes 2π, which is the form above.
Assumptions
- Two complete concentric spheres of uniform water; the stem and filler port are ignored.
- The meter's conductivity, uniform and at DC — see the tubular leak calculation.