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This Book in PDF - Gary North

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INTRODUCTIONThy raiment waxed not old upon thee, neither did thyfoot swell, thesefortyyears (Deut. 8:4).Andye shall serve the LORDyour God, and he shall bless thy bread, andthy water; and I will take sickness away from the midst of thee. Thereshall noth<strong>in</strong>g cast their young, nor be barren, <strong>in</strong> thy land: the number ofthy days I willfulfil (Ex. 23:25-26).The first law of thermodynamics states that the total of "matterenergy"<strong>in</strong> the universe is constant throughout eternity, or at leastafter the "Big Bang" (the evolutionists' version of creation). The secondlaw of thermodynamics states that useful energy is either constant(equilibrium conditions)1 or decreas<strong>in</strong>g (k<strong>in</strong>etic energy) <strong>in</strong> theuniverse as a whole. Useful energyfor the universe as a whole thereforecan never <strong>in</strong>crease. (The underly<strong>in</strong>g assumption of the second law isthat the universe itself is a closed system, someth<strong>in</strong>g like a giant conta<strong>in</strong>er.Without this crucial assumption, the second law of thermodynamicsloses its status as a universal law.)We read: "Thy raiment waxed not old upon thee, neither did thyfoot swell, these forty years" (Deut. 8:4). Thus, any consistent scientificapplication of the second law of thermodynamics to this versewould have to assert that God must have drawn energy from someexternal source <strong>in</strong> order to produce this local overcom<strong>in</strong>g ofentropy'seffects. Perhaps God <strong>in</strong> some way rechanneled energy from the sunthat otherwise would have been dissipated <strong>in</strong>to space, or <strong>in</strong>to the1. A system is <strong>in</strong> equilibrium when its components are not mov<strong>in</strong>g <strong>in</strong> any particulardirection. When a gas is <strong>in</strong> equilibrium <strong>in</strong> a conta<strong>in</strong>er, its molecules are bounc<strong>in</strong>grandomly aga<strong>in</strong>st the walls of the conta<strong>in</strong>er. In theory, no heat from outside theconta<strong>in</strong>er passes through to the gas <strong>in</strong>side, and no heat from the gas <strong>in</strong>side passesduough the conta<strong>in</strong>er's walls to the outside. The random bounc<strong>in</strong>g of the moleculesof the gas does not produce measurable changes- heat, pressure- <strong>in</strong> the gas, takenas a unit.1

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