- Mechanical Work
W = - Pext (ΔV) [during expansion] - First Law of Thermodynamics
ΔE = q + W
ΔE = q - PΔV - Adiabatic Change
- Isochoric Change
ΔV = 0
W = PΔV = 0
ΔE = q + W = q - Cyclic Change (reversible)
ΔE = 0
q = -W = PΔV
q = -Wmax = P∫dV - Isothermal reversible Expansion
ΔH = ΔE = 0 (internal energy is a function of temperature)
q = -Wmax = 2.303 nRT log( V2 / V1) = 2.303 nRT log( P1 / P2)
ΔH = ΔE + ΔngRT - Joule - Thompson coefficient
(i) For cooling , u > 0 (-ve sign)
(ii)For heating , u < 0 (+ve sign) - Second Law of Thermodynamics
Efficiency of the Carnot engine = η =q2 - q1q2=T2 - T1T2= 1 -T1T2
q2 = heat absorbed by engine
q1 = heat lost to sink - Entropy Change
ΔStotal = ΔSsystem + ΔSsurrounding
ΔSfusion =ΔHfusionTfusion; ΔSvapour =ΔHvapourTvapour - Gibb's Free Energy (G)
ΔG = G2 - G1
ΔG = ΔH - TΔS (Gibb's Helmholtz equation)
ΔG < 0 (means spontaneous process)
ΔG > 0 (means non-spontaneous process)
ΔG = 0 (means system is at equilibrium) - Kirchoff's EquationΔH2 - ΔH1T2 - T1= ΔCp andΔE2 - ΔE1T2 - T1= ΔCv
where , ΔCp = ∑Cp(products) - ∑Cp(reactants) and ΔCv = ∑Cv(products) - ∑Cv(reactants) - Degree of Dissociation (x)
x =D - dd=Mt - MoMo
where , D = theoretical V.D. and d = observed V.D. - pH of a solution
pH = -log[H3O+]
pOH = -log[OH-]
pH + pOH = pKW = 14 - Isothermal (reversible)
ΔS = 2.303 nR log (V2 / V1)
at constant pressure ,
ΔS = 2.303 Cp log10 (T2 / T1)
For vaporization ,
ΔS =ΔHvapTbp
ΔGo = - nFE0cell - Sign Convention
- If work is done on the system , W is +ve.
- If work is done by the system , W is -ve.
- If heat is absorbed by the system , or ΔH is +ve.
- If heat is given out by the system , q or ΔH is -ve.
- If energy is absorbed by the system , i.e. internal energy increases , ΔE is +ve.
- If energy is released i.e., internal energy of the system decreases , ΔE is -ve.
- Heat Capacity
(i) Heat capacity at constant volume , CV = [ ∂E / ∂T ]V
(ii) Heat capacity at constant pressure , Cp = [ ∂H / ∂T ]p
For an ideal gas , Cp - Cv = R - Heat of Reaction
ΔH = ∑ H(p) - ∑ H(R)
For exothermic reaction : ∑ H(p) < ∑ H(R) (∴ Δ is -ve)
For endothermic reaction : ∑ H(p) > ∑ H(R) (∴ Δ is +ve)
Heat change at constant pressure = qp = ΔH
Heat change at constant volume = qv = ΔH
ΔH = ΔU + PΔV
ΔH = ΔU + Δn(g)RT
If,
Δn(g) = 0 , ΔH = ΔU
Δn(g) > 0 , ΔH > ΔU
Δn(g) < 0 , ΔH < ΔU - Clausis - Clapeyron Equation
where ΔHv = molar heat of vapourisation- Calorific Value is the amount of heat evolved when one gram of fuel as food is burnt in the presence of air or excess of oxygen.
- Joule's Relationship between work done (w) and heat produced (H)
W α H or W = JH
where J = mechanical equivalent of heat ; J = 4.184 JCal-1 - S1 and S2 are solubility at temperature T1 and T2 respectively
Sunday, March 30, 2014
THERMODYNAMICS
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