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Ideal Gas Law Physics 313 Professor Lee Carkner Lecture 10
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Exercise #9 -- Chicken Cool to -2.8C: Q 1 = cm T = (3.32)(50)(8.8) = Phase change: Q 2 = Lm = (247)(5) = Cool to -18 C: Q 3 = (1.77)(50)(15.2) = Cool box to -18 C: Q 4 = (1.4)(1.5)(24) = Sum all heats: Q T = Q 1 + Q 2 + Q 3 + Q 4 = Most heat lost for phase change
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Ideal Gas What is an ideal gas? The properties converge to common values as P goes to zero An ideal gas is any gas at the limit of zero pressure
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Approaching Zero Pressure The equation of state of a gas depends on T, P and V We know that for constant V: Can express Pv relationship by virial expansion: Experiment reveals that for constant T: A is function of T only
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Equation of State: Ideal Gas Combining equations We can write the constant part of this equation as: The equation of state for any gas as pressure approaches zero is:
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Internal Energy What does the internal energy depend on? For a real gas U is dependant on P ( U/ P) T = 0 [as P goes to 0]
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Ideal Gas Relations For an ideal gas: PV = nRT Internal energy is a function of the temperature only
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Ideal and Real Gas Real gases deviate from ideal ones with pressure We can express the deviation from ideal gas behavior with the compressibililty factor, Z For an ideal gas: Pv = RT For a real gas: Pv = ZRT z = 1 for ideal gasses
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Critical Point What determines if a gas is at high or low pressure? The point where there is no difference between liquid and gas The critical point is defined by a critical volume, pressure and temperature (V C,P C,T C )
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Gas Mixtures e.g. air How is P,V and T for the mixture related to the properties of the individual gasses?
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Mixture Laws Dalton’s Law: P m = P i (T m,V m ) Amagat’s Law: V m = V i (T m,P m ) Strictly true only for ideal gases
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Mixture Properties Z m = y i Z i Where y i is the mole fraction (y i = n i /n m ) P m V m = Z m n m RT m It may be hard to determine Z i
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First Law for Ideal Gas dU = dQ + dW dW = -PdV At constant volume: Since U depends only on T: dQ = C V dT + PdV
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Constant Pressure PV = nRT dQ = C V dT + nRdT -VdP At constant pressure: Molar heat capacity: c P = c V + R
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Forms of the First Law For an ideal gas: dU = dQ =
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Heat Capacities For an ideal gas: For monatomic gas: For any gas:
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