Equations Topic 5/15 Flashcards
Heat transfer equation
Q = mcΔT => ΔH = mcΔT / n
where
Q = heat transfer
m = mass
c = heat capacity
ΔT = change in temperature
ΔH = change in enthalpy
n = number of moles
Change in enthalpy at STP (enthalpies of formation)
ΔHθ = ΣHθf (product) - ΣHθf (reactant)
where
ΔHθ = change in enthalpy at STP
ΣHθf = sum of the enthalpies of formation
Change in enthalpy at STP (bond enthalpies)
ΔHθ = ΣE (broken) - ΣE (formed)
where
ΔHθ = change in enthalpy at STP
ΣE = sum of enthalpies
Entropy
ΔSθreaction = ΣSθ (product) - ΣSθ (reactant)
where
ΔSθr = change in entropy at STP
ΣSθ = sum of entropies at STP
Spontaneity
ΔG = ΔH - TΔS
where
ΔG = change in Gibbs free energy
ΔH = change in enthalpy
T = temperature
ΔS = change in entropy
**If G is negative, the reaction is spontaneaous
Change in enthalpy (with number of moles)
ΔH = Q / n
where
ΔH = enthalpy change (J mol^-1)
Q = energy (kilojoules / kJ)
n = number of moles (mol)
Lattic enthalpy ionic model
ΔHølat = (Knm) / (Rx n+ + Ry m-)
where
K = a constant that depends on the geometry of the lattice
n & m = are charges of the ions
R = radius of each respective ion
X = metal
Y = non-metal
Equation that links solution enthalpy, lattice enthalpy and enthalpies of hydration, for any ionic compound.
ΔHøsol (XY) = ΔHølat (XY) + ΔHøhyd (X+) + ΔHøhyd (Y−)
Entropy change for surroundings
ΔS (surroundings) = - ΔH (system) / T; unit: J K^-1 mol^-1
Calculating total entropy change
ΔS (total) = ΔS (system) + ΔS (surroundings) > 0
(substituting entropy change for surroundings)
ΔS (total) = ΔS (system) + - ΔH (system) / T > 0
Exothermic reactions
Increase the entropy of the surroundings as heat is dispersed into the surroundings. This clearly allows for ΔS (total) to be greater than zero, as entropy increases.
Endothermic reactions
There is a decrease in the entropy of the surroundings, but this is compensated for by a greater increase in the entropy of the system, once again allowing for ΔS (total) to be greater than zero.
The Second Law of Thermodynamics
States that:
- total entropy of an isolated system can never decrease.
- total entropy of an isolated system is constant only if all processes are reversible.
- this system will spontaneously move to a state of maximum entropy.