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I don't think that osmotic pressure establishes entropy as a force. And there are a few reasons why:1) The most important part of establishing an osmotic pressure is the mechanism of allowing only one substance to cross from one chamber to another: Whether it is a semipermeable membrane that allows water to cross, but not some other type of dissolved species, or a shared headspace that allows volatile compounds to exchange between the chambers without allowing the exchange of non-volatile species. What drives the equilibrium is not necessarily entropy, but the sorting mechanism that is applied.For instance let us imagine two chambers separated by a water-permeable membrane. One chamber contains a 1 molal solution of compound X in H2O, while the other contains pure H2O. Using colligative equations, we find that there should be an osmotic pressure of 24.6 atmospheres at 300 K (pressure in atm = 0.0821 * T in Kelvin * molality of dissolved species). If compound X is something like pyridine or t-butanol, this is perfectly valid. But what if compound X is D2O? The entropy of mixing is unchanged, but D2O can cross the barrier at the same rate as H2O, so there will be 0 osmotic pressure!In essence, there is one characteristic of the solute that does matter, and that is the extent to which is is capable of moving between chambers.2) The source of the energy is thermal. You can think of the semi-permeable barrier as a device analogous to a valve or a winch or one of those watches that charges itself using the mechanical energy of the wearer's pace. Each of these can allow random or multi-directional motions to be unidirectional. There is nothing magical involved, and all of the energy can be traced back to electrostatic or gravitational sources (or one of the other two forces, but this is rarer), so there is no 5th force required.
The entropy of a system (S) is related to the number of states (W) the system can be in by S = k*log(W).A gas will expand to fill an available vacuum because each particle can be in more different locations (more states). By analogy, one might expect that space could expand to give the gas more possible states.But the question is, as space expands, is it in such a way that there are actually more states available? If we imagine the universe as an image made of pixels (more pixels = more information = more entropy) as the image expands, is it adding pixels, or are the pixels getting bigger? If it is the latter, then I would not expect this process to be driven entropically.
Another question is, if we assume that expansion is adding pixels, does the change in entropy rely on there being matter that can form multiple states? One might expect that regions of the universe with more matter to expand more rapidly than empty regions...
Again this raises an issue regarding the linear nature of the expansion. You cannot avoid the results of Hubble's observations. What is your opinion of a link between entropy and expansion?
The entropy of a system (S) is related to the number of states (W) the system can be in by S = k*log(W).A gas will expand to fill an available vacuum because each particle can be in more different locations (more states). By analogy, one might expect that space could expand to give the gas more possible states.But the question is, as space expands, is it in such a way that there are actually more states available? If we imagine the universe as an image made of pixels (more pixels = more information = more entropy) as the image expands, is it adding pixels, or are the pixels getting bigger? If it is the latter, then I would not expect this process to be driven entropically.Another question is, if we assume that expansion is adding pixels, does the change in entropy rely on there being matter that can form multiple states? One might expect that regions of the universe with more matter to expand more rapidly than empty regions...
Quote from: chiralSPO on 05/02/2016 15:26:10The entropy of a system (S) is related to the number of states (W) the system can be in by S = k*log(W).A gas will expand to fill an available vacuum because each particle can be in more different locations (more states). By analogy, one might expect that space could expand to give the gas more possible states.But the question is, as space expands, is it in such a way that there are actually more states available? If we imagine the universe as an image made of pixels (more pixels = more information = more entropy) as the image expands, is it adding pixels, or are the pixels getting bigger? If it is the latter, then I would not expect this process to be driven entropically.Another question is, if we assume that expansion is adding pixels, does the change in entropy rely on there being matter that can form multiple states? One might expect that regions of the universe with more matter to expand more rapidly than empty regions...The idea of states W for entropy is useful because it tells use entropy is not necessarily randomness. For example, say we start a hydrogen molecule H2. There is a certain amount of energy needed to break the covalent bond; overcome the EM forces to form two atoms of hydrogen; 104 kcal/mole. If add smaller amounts of energy to increase entropy, but not enough energy to break the bond, than more states W of the hydrogen molecule will appear The entropy increase can be defined as vibrational, rotational, translational, torsional and bending states for the hydrogen molecule. These states of entropy are not exactly random, but define distinct classes of quantized energy levels that are the same for any H2. This gives us a unique H2 fingerprint. These extra entropic states W add potential energy to the hydrogen molecule and place different strains on the EM force based covalent bond, but not enough to break the bond. In this case, the entropy is defining force opposite the EM force but in 3-D. This entropic force is translating, pushing, pulling, bending, twisting and rotating the hydrogen adding potential to the EM force. This is simpler to way pressure impacts 3-D surfaces; from all sides. Osmotic pressure extends this. We may call a very specific instant of these five sub-states, random. But in the long term, these states will come under the umbrella of five classes of motion, each with certain quantum states. Entropy is about long term character as well as the short term uniqueness, with both allowing distinct variety in the four base forces; 3-D swiss army knife anti-force. For example, if we added heat to the core of the earth, new states of interaction will appear among all the materials mediated in 3-D by pressure.