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Old 02-17-2010, 02:05 AM
witsend witsend is offline
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And then the next question? What form would those dipoles take once they are outside the whole of the field? To get to this answer I need to digress. Just for now - imagine that we have a machine that throws stones. Here's the rule. The force of the throw is constant. And there are no extraneous conditions of air resistance or wind or anything at all. It throws these stones inside a vacuum. That means, that all things being equal, then the bigger the stone the shorter the distance thrown. And conversely, the smaller the stone the further the distance thrown. That's logical. I'll get back to this point. But what I actually need to first concentrate on is an 'interactive constraint'. If the stone were too big then the machine could not lift it to throw it. And in the same way, if the stone was too small then the machine could not detect it to throw it. That's what the model refers to as a boundary constraint. The condition of size would threby limit the interactive capability of the machine. In the same way I'm proposing that if these little magnets in a broken string - tumbled out of the field and congregated into vast nebulae then what makes them visible and would it then be 'out of range' or 'outside the boundary constraint' of the magnetic dipoles in the field surrounding the nebula?
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Last edited by witsend; 02-17-2010 at 03:43 AM.