Equations Topic 5/15 Flashcards

1
Q

Heat transfer equation

A

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

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2
Q

Change in enthalpy at STP (enthalpies of formation)

A

ΔHθ = ΣHθf (product) - ΣHθf (reactant)

where
ΔHθ = change in enthalpy at STP
ΣHθf = sum of the enthalpies of formation

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3
Q

Change in enthalpy at STP (bond enthalpies)

A

ΔHθ = ΣE (broken) - ΣE (formed)

where
ΔHθ = change in enthalpy at STP
ΣE = sum of enthalpies

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4
Q

Entropy

A

ΔSθreaction = ΣSθ (product) - ΣSθ (reactant)

where
ΔSθr = change in entropy at STP
ΣSθ = sum of entropies at STP

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5
Q

Spontaneity

A

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

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6
Q

Change in enthalpy (with number of moles)

A

ΔH = Q / n

where
ΔH = enthalpy change (J mol^-1)
Q = energy (kilojoules / kJ)
n = number of moles (mol)

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7
Q

Lattic enthalpy ionic model

A

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

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8
Q

Equation that links solution enthalpy, lattice enthalpy and enthalpies of hydration, for any ionic compound.

A

ΔHøsol (XY) = ΔHølat (XY) + ΔHøhyd (X+) + ΔHøhyd (Y−)

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9
Q

Entropy change for surroundings

A

ΔS (surroundings) = - ΔH (system) / T; unit: J K^-1 mol^-1

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10
Q

Calculating total entropy change

A

ΔS (total) = ΔS (system) + ΔS (surroundings) > 0
(substituting entropy change for surroundings)

ΔS (total) = ΔS (system) + - ΔH (system) / T > 0

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11
Q

Exothermic reactions

A

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.

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12
Q

Endothermic reactions

A

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.

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13
Q

The Second Law of Thermodynamics

A

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.
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