junglelord wrote:I think its a bit ingenous to suggest that the ropes can account for heat. Sorry, but I fail to see how that translates.
What about zero point, super cold atoms? They have more ropes, being closer together, while as you say, the ropes dissipate at the inverse square, so how could a gas, being further apart, have more ropes and heat?
Firstly, I think you mean [url2=
http://dictionary.reference.com/search?q=disingenuous]disingenuous[/url2].
Secondly, to answer your question, the # of ropes (N) per unit volume (V) around an object decreases as the inverse square of the distance (D) from that object, but the torsion along one rope propagates undiminished (or undiminished enough that it is negligible for this particular discussion). So if I am 1 unit distance from the object under study I may have 10^9 ropes intersecting my detector. Each one has a frequency f (f = # of links in a rope n per unit length L). The "heat" or "energy" I detect is proportional to 10^9*f. If I move one unit distance further away the # of ropes converging on my detector is now 2.5E8 and the "heat" or "energy" I detect is proportional to 2.5E8*f.
I think the difficulty/confusion you're having is to distinguish between "geometric" intensity density Ig=(N/V), which goes as the inverse square of the static distance D, and "invariant" total intensity It=N*f.
"Cold" just means the object's ropes are at a lower frequency, and vice versa for "hot". A very very hot object can feel very cold if you are far away. A very cold object can feel hot if you are very close to it. Case in point, the sun. Standing on Pluto the sun seems very cold. Another case in point, my stove. Standing very close to it, it feels hotter than the sun. However I know that N(sun)>>N(stove), even if f is the same for both, so I know that It(sun)>>It(stove) even though Ig(sun)<Ig(stove) where I happen to be standing.
Another point to make, gas molecules are considered "hot" because they are moving fast. This is more of a human convention than anything else, because atoms that move fast tend to "feel hot". We could just as well say that thorium (234) is "hot" because it emits "gamma rays", although it certainly would not "feel hot".