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A Brief Review of Thermodynamics
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Internal Energy and the First Law The infinitesimal change in the internal energy For a general process The First Law of Thermodynamics
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The Constant Volume Heat Capacity Define the constant volume heat capacity, C V
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Enthalpy We define the enthalpy of the system, H
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The Constant Pressure Heat Capacity Define the constant pressure heat capacity, C P
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Thermodynamic Definition Spontaneous Process – the process occurs without outside work being done on the system.
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Mathematical Definition of Entropy The entropy of the system is defined as follows
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The Fundamental Equation of Thermodynamics Combine the first law of thermodynamics with the definition of entropy.
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The Temperature dependence of the Entropy Under isochoric conditions, the entropy dependence on temperature is related to C V
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Entropy changes Under Constant Volume Conditions For a system undergoing an isochoric temperature change For a macroscopic system
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The Temperature dependence of the Entropy Under isobaric conditions, the entropy dependence on temperature is related to C P
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Entropy changes Under Constant Pressure Conditions For a system undergoing an isobaric temperature change For a macroscopic system
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The Second Law of Thermodynamics The second law of thermodynamics concerns itself with the entropy of the universe ( univ S). univ S unchanged in a reversible process univ S always increases for an irreversible process
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The Third Law of Thermodynamics The Third Law - the entropy of any perfect crystal is 0 J /(K mole) at 0 K (absolute 0!) Due to the Third Law, we are able to calculate absolute entropy values.
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Combining the First and Second Laws From the first law
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Pressure Volume and Other Types of Work Many types of work can be done on or by chemical systems. Electrical work. Surface expansion. Stress-strain work. dw=-P ext dV+dw a where dw a includes all other types of work
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The General Condition of Equilibrium and Spontaneity For a general system
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Isothermal Processes For a systems where the temperature is constant and equal to T surr
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The Helmholtz Energy Define the Helmholtz energy A A(T,V) =U – TS Note that for an isothermal process dA dw A w For an isochoric, isothermal process A 0
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The Properties of A The Helmholtz energy is a function of the temperature and volume
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Isothermal Volume Changes For an ideal gas undergoing an isothermal volume change
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Isothermal Processes at Constant Pressure For an isothermal, isobaric transformation
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The Gibbs Energy Define the Gibbs energy G G(T,P) =U – TS+PV Note that for an isothermal process dG dw a G w a For an isothermal, isobaric process G 0
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The Properties of G The Gibbs energy is a function of temperature and pressure
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Isothermal Pressure Changes For an ideal gas undergoing an isothermal pressure change
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Temperature Dependence of A Under isochoric conditions
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Gibbs Energy Changes As a Function of Temperature The Gibbs energy changes can be calculated at various temperatures
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The Chemical Potential Define the chemical potential = G/n
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Gibbs Energy and Spontaneity sys G < 0 - spontaneous process sys G > 0 - non-spontaneous process (note that this process would be spontaneous in the reverse direction) sys G = 0 - system is in equilibrium
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Applications of the Gibbs Energy The Gibbs energy is used to determine the spontaneous direction of a process. Two contributions to the Gibbs energy change ( G) Entropy ( S) Enthalpy ( H) G = H - T S
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Thermodynamics of Ions in Solutions Electrolyte solutions – deviations from ideal behaviour occur at molalities as low as 0.01 mole/kg. How do we obtain thermodynamic properties of ionic species in solution?
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For the H + (aq) ion, we define f H = 0 kJ/mole at all temperatures S = 0 J/(K mole) at all temperatures f G = 0 kJ/mole at all temperatures
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Activities in Electrolyte Solutions For the following discussion Solvent “s” Cation “+” Anion “=“ Consider 1 mole of an electrolyte dissociating into + cations and - anions G = n s s + n = n s s + n + + + n - - Note – since = + + - = + + + - -
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The Mean Ionic Chemical Potential We define = / We now proceed to define the activities = + RT ln a + = + + RT ln a + - = - + RT ln a - = + RT ln a
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The Relationship Between a and a Since = / = + RT ln a = ( + RT ln a ) Since = / This gives us the relationship between the electrolyte activity and the mean activity (a ) = a
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The Relationship Between a , a - and a + We note that = + + + - - and = / This gives us the following relationship ( + RT ln a ) = + ( + + RT ln a + ) + - ( - + RT ln a - ) Since = + + + - - (a ) = (a + ) + (a - ) -
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Activities in Electrolyte Solutions The activities of various components in an electrolyte solution are defined as follows a + = + m + a - = - m - a + = + m + As with the activities ( ) = ( + ) + ( - ) - (m ) = (m + ) + (m - ) -
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The Chemical Potential Expression This can be factored into two parts The ideal part Deviations from ideal behaviour
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KCl CaCl 2 H 2 SO 4 HCl LaCl 3 Activity Coefficients As a Function of Molality Data obtained from Glasstone et al., Introduction to Electrochemistry, Van Nostrand (1942). CRC Handbook of Chemistry and Physics, 63 rd ed.; R.C. Weast Ed.; CRC Press, Boca Raton, Fl (1982).
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Estimates of Activity Coefficients in Electrolyte Solutions The are a number of theories that have been proposed to allow the theoretical estimation of the mean activity coefficients of an electrolyte. Each has a limited range of applicability.
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u This is valid in the up to a concentration of 0.010 molal! The Debye Hűckel Limiting Law Z + = charge of cation; z - = charge of anion
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Debye Hűckel Extended Law This equation can reliably estimate the activity coefficients up to a concentration of 0.10 mole/kg. B = 1.00 (kg/mole) 1/2
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The Davies Equation This equation can reliably estimate the activity coefficients up to a concentration of 1.00 mole/kg. k = 0.30 (kg/mole)
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