Hahahahahaha. I've quite enjoyed watching you two battle it out over various threads
@
DiabolusInMusic - I really feel that your heart is in the right place, and I think you've been genuinely very helpful by posting this shielding thread. Practically, pragmatically, your approach to shielding may well be absolutely fine in the vast majority of cases.
The problem is, you have a fundamentally incorrect notion of what "resistance" is, and what the shielding is doing (and why it's important that it's very conductive, and therefore measures a low (ideally zero - note, this is the
mathematical/scientific use of the word "ideal") resistance.
Like I said, this actually doesn't matter if everything works. The problem comes when it doesn't "just work", and you need to have a way to diagnose the issue. Measuring resistance, and making educated inferences from the results is the most effective way to do this.
Please, please don't take this next request as an insult - I think you can really help a lot of people here on TB (and probably in RL too), but take a moment to familiarise yourself with some electronics theory. This is a great start:
http://en.wikipedia.org/wiki/Electrical_resistance_and_conductance
Some key excerpts:
The electrical resistance of an DiabolusInMusic is the opposition to the passage of an electric current through that conductor. The inverse quantity is electrical conductance, the ease with which an electric current passes. Electrical resistance shares some conceptual parallels with the mechanical notion of Invalid Link Removed. The Invalid Link Removed unit of electrical resistance is the ohm (Ω).
Substances electricity can flow through are called Invalid Link Removed. Conductors are made of high-Invalid Link Removed materials such as metals, in particular copper and aluminium.
Further down, you'll find the typical resistance of 1 meter of copper wire which is 1mm in diameter is 0.02 ohms. Copper tape is a little thinner than this, but we are also making shorter runs, and it is much "wider" that 1mm (it's the cross-sectional area [roughly] which is important).
So yes, copper will never
truly have a 0 ohm resistance - only superconductors near absolute zero (273.15°C or −459.67°F) can approach this.
However, for our application (and as far as our meters can read), it should be "notionally" zero.
This is
extremely important in order for the shield to work. If you don't believe me, think about the resistance of wood - millions (billions? I don't even know) of ohms. If resistance was good, why does the wood of the bass not act as a super-awesome shield?
I might also address one more slight misconception you seem to have:
I know we are adding a conductive material that indicates a resistance when you put a meter to it, hence adding resistance.
EVERY material in the entire world has a resistance. For most materials, this is quite high. For some special ones, it is very low (relatively). Copper is one of these special cases. Thus:
Copper has the highest resistance.
Is false.
Now, if you choose to really get a handle on this stuff, your knowledge of the world will have greatly increased, but more importantly, your knowledge of bass shielding will be (essentially) complete, and you'll be a valuable resource to the TB community and the world.
I'd like that. You seem like a kind dude.
Hopefully this post has been helpful and clarifying. We cool, right?
--Moley