chem20212 - electrochemistry

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electrochemistry, quantum, electronic structure

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74 Terms

1
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equation for molarity

c = mol dm-3

V = dm3

<p>c = mol dm-3</p><p>V = dm3</p>
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molality equation

m = mol kg-1 M = molar mass kg mol-1

<p>m = mol kg-1 M = molar mass kg mol-1</p>
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mol fraction equation

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chemical potential equation of an ideal gas in pure phase

μ = J mol-1 G = J

  • chemical potential is the molar gibbs of the pure phase at constant p,T if it behaves ideally

<p>μ = J mol-1 G = J</p><ul><li><p>chemical potential is the molar gibbs of the pure phase at constant p,T if it behaves ideally </p></li></ul><p></p>
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chemical potential and gibbs free energy at equilibrium

  • ΔG = 0 at equilibrium therefore chemical potential is constant

<ul><li><p>ΔG = 0 at equilibrium therefore chemical potential is constant </p></li></ul><p></p>
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chemical potential of a real gas - expansion at constant T

μ = J mol-1 p = Pa = J m-3

<p>μ = J mol-1 p = Pa = J m-3</p>
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total gibbs energy before mixing ideal gases

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total gibbs energy after mixing ideal gases

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total Gibbs energy of mixing ideal gases eq. how does this prove spontaneity

  • shows that mixing ideal gases is always spontaneous because ΔG = -ve

  • xi < 1 and nRT = +ve → -ve + +ve = -ve

<ul><li><p>shows that mixing ideal gases is always spontaneous because ΔG = -ve </p></li><li><p> xi &lt; 1 and nRT = +ve  → -ve + +ve = -ve </p></li></ul><p></p>
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Gibbs energy of mixing ideal gases at not equal pressure eq

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total entropy of mixing

  • the bottom part is the derivation

<ul><li><p>the bottom part is the derivation </p></li></ul><p></p>
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free gibbs energy equation

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chemical potential of real gases

φ = fugacity → its an effective pressure, correcting for non ideality

  • deviation between chemical potential of ideal gases and real gases is due to attractive Van Der Waal interactions

<p>φ = fugacity → its an effective pressure, correcting for non ideality </p><ul><li><p>deviation between chemical potential of ideal gases and real gases is due to attractive Van Der Waal interactions </p></li></ul><p></p>
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chemical potential of ideal solutions

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raoults law eq and argument

  • argued that mol fraction in solution reduces vapour pressure of certain mixtures from the pressure in pure phase. shown in eq

  • he takes the assumption that components in solution will behave like ideal gases → mixing of gases is driven by entropy so ΔH mix = 0 → no change in interactions before and after mixing

  • this will only be approximately accurate if A is surrounded by A ( A being solvent)

<ul><li><p>argued that mol fraction in solution reduces vapour pressure of certain mixtures from the pressure in pure phase. shown in eq</p></li><li><p>he takes the assumption that components in solution will behave like ideal gases → mixing of gases is driven by entropy so <span>ΔH mix = 0 → no change in interactions before and after mixing </span></p></li><li><p> this will only be approximately accurate if A is surrounded by A ( A being solvent)</p></li></ul><p></p>
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chemical potential of solution according to Raoult’s law

  • assumption is made that components in solutions behave like real ideal gases

<ul><li><p>assumption is made that components in solutions behave like real ideal gases </p></li></ul><p></p>
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Henrys law

K = empirical constant for pure component B

  • about ideal dilute solution

  • implies interactions before / after mixing are different → will be approximately valid when B is surrounded by other molecules (A) . B being the solute

<p>K = empirical constant for pure component B </p><ul><li><p>about ideal dilute solution </p></li><li><p>implies interactions before / after mixing are different → will be approximately valid when B is surrounded by other molecules (A) . B being the solute </p></li></ul><p></p>
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what does it mean by colligative properties

  • important properties of liquid solution → Tm, Tf, b.p elevation

  • this is dependent on the amount of solute not its identity

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what are the two arguments for why chemical potential in pure phase > actual chemical potential

  1. thermodynamic origin of solution stability

    • solution formation ΔG = -ve

    • in pure liquid ΔS is increased by evaporation → more favourable to be in evaporated state

    • in solution the motion is more random (ΔS is higher than in pure phase) → lower thermodynamic tendency to evaporate

  2. semi quantitative argument

    • chemical potential eq for ideal solution is μA = μA* + RTlnχA

    • we know μA < μA* because the latter part of the eq is -ve

    • we know at equilibrium μA(l) = μA*(g)

    • if μA is lower in solution, we need higher temp to make it boil and lower temp to make it freeze

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<p>what happens to this over time</p>

what happens to this over time

  • diluting the solute is favourable, therefore pressure increases in solution compartment

  • called osmotic pressure

  • driven by thermodynamics

<ul><li><p>diluting the solute is favourable, therefore pressure increases in solution compartment </p></li><li><p>called osmotic pressure</p></li><li><p>driven by thermodynamics </p></li></ul><p></p>
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osmotic pressure equation for dilute solution (when xB v. small)

Vm = molar volume

  • apply this to water purification

  • if p > Π then water will be squeezed out

<p>Vm = molar volume</p><ul><li><p>apply this to water purification</p></li><li><p>if p &gt; <span>Π then water will be squeezed out </span></p></li></ul><p></p>
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change in boiling temperature eq

  • can switch xB with mB because xB < < 1

<ul><li><p>can switch xB with mB because xB &lt; &lt; 1 </p></li></ul><p></p>
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change in freezing temperature eq

  • can switch xB with mB because xB < < 1

<ul><li><p>can switch xB with mB because xB &lt; &lt; 1 </p></li></ul><p></p>
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why are alcohols / water and electrolytes not ideal

  • ideality means interactions before = after mixing

  • alcohols and water have H bonding when mixed

  • electrolytes conduct electricity when dissolved → display strong water - ion interactions

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compare strong and weak electrolytes

  1. strong - completely dissociate → degree of dissociation is independent of concentration

  2. weak - partially dissociate → degree of dissociation is a function of concentration

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what is the definition of the gibbs energy of solvating an ion

  • the energy required for 1 mol of gaseous ion to become 1 mol of solvated ion

  • its difficult to measure solvation parameters for individual ions → because other interactions occur

<ul><li><p>the energy required for 1 mol of gaseous ion to become 1 mol of solvated ion </p></li><li><p>its difficult to measure solvation parameters for individual ions →  because other interactions occur </p></li></ul><p></p>
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Borns approach to ion solvation - gibbs energy in vacuum

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Borns approach t o ion solvation - gibbs energy of solvent

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Born’s approach to ion solvation - Gibbs energy of solvation

  • meaning it’ll always be favourable for ions to solvate

  • as the εr increases ΔG solvation will become increasingly -ve

<ul><li><p>meaning it’ll always be favourable for ions to solvate </p></li><li><p>as the <span>εr increases ΔG solvation will become increasingly -ve </span></p></li></ul><p></p>
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how does transport in electrolytes work

  • you can force ions to move in a certain direction if you apply a potential difference between two electrodes

  • this produces an electric field

  • charge carriers migrate to the oppositely charged electrode → cations to cathode , anions to anode

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ohms law

V = voltage

I = current (A)

R = resistance ( Ω ≡ V A−1

<p>V = voltage </p><p>I = current (A) </p><p>R = resistance ( <span style="font-family: &quot;Times New Roman&quot;, serif">Ω ≡ V A<sup>−1</sup></span></p><p></p>
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conductance eq

G = conductance

R = resistance (Ω)

k = conductivity (Ω−1 m−1)

A = area (m2)

l = length (m)

<p>G = conductance</p><p>R = resistance (<span>Ω)</span></p><p><em>k</em><span style="font-family: &quot;Times New Roman&quot;, serif"> = conductivity (Ω<sup>−1</sup> m<sup>−1</sup>)</span></p><p><span style="font-family: &quot;Times New Roman&quot;, serif"><em>A = </em>area (m<sup>2</sup>)</span></p><p><span style="font-family: &quot;Times New Roman&quot;, serif"><em>l = </em>length (m)</span></p>
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conversion from ohm to siemens

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conductance definition

how easily the current will flow through a material

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conductivity definition

  • intrinsic ability of a material to conduct electricity

  • it increases with concentration increasing. but as conc increases the conductivity will increase by a smaller amount

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molar conductivity eq

<p></p>
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Kohlrauch eq for molar conductivity

  • molar conductivity decreases as conc increases because interactions with ions. the more interactions the less it can conduct as they are slowed down

<ul><li><p>molar conductivity decreases as conc increases because interactions with ions. the more interactions the less it can conduct as they are slowed down</p></li></ul><p></p>
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limiting molar conductivity eq

Λ0 = limiting molar conductivity, i.e. at infinite dilution (m2 Ω−1 mol−1)

ν = stoichiometric factor

λ = molar conductivity of ionic equivalents (m2 Ω−1 mol−1)

<p><span>Λ<sup>0</sup></span><span style="font-family: &quot;Times New Roman&quot;, serif"> = limiting molar conductivity, i.e. at infinite dilution (m<sup>2</sup> </span><span>Ω</span><span style="font-family: &quot;Times New Roman&quot;, serif"><sup>−1</sup> mol<sup>−1</sup>)</span></p><p><span>ν</span><span style="font-family: &quot;Times New Roman&quot;, serif"><em> = </em>stoichiometric factor</span></p><p><span>λ </span><span style="font-family: &quot;Times New Roman&quot;, serif">= molar conductivity of ionic equivalents (m<sup>2</sup> Ω<sup>−1</sup> mol<sup>−1</sup>)</span></p>
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what does the limit of infinite dilution look like on a graph for strong and weak electrolytes

  • strong → the electrolyte interactions that sloe down the conductivity as conc increases

  • weak → the dissociation of ions is incomplete and its also a function of conc

<ul><li><p>strong → the electrolyte interactions that sloe down the conductivity as conc increases </p></li><li><p>weak → the dissociation of ions is incomplete and its also a function of conc </p></li></ul><p></p>
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what can you work out with conductivity

  • measuring the degree of dissociation of weak electrolytes

  • limiting conductivity values relate to ion mobility

  • relating ion mobility to effective size of ions in solution → the ion + solvation shell

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osmotic pressure equation for non dilute solution (when xB bigger )

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chemical potential of liquid solution that doesn’t behave ideally

γ = activity coefficient

m = molality mol kg-1

<p><span>γ = activity coefficient </span></p><p><span>m = molality mol kg-1 </span></p>
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what does the activity of a solute aB tell us

  • the effective molality of the solute → correcting for solute-solute interaction

  • when RTlnγB = 0 the solution will be ideal → this would only be the case in very dilute solution

  • in electrolytes the cations surround the anions forming ionic atmospheres → stabilising the solution

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Debye-Huckle law - activity coefficient eq

unitless

<p>unitless </p>
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ionic strength eq

unitless

<p>unitless</p>
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what does the Debye-Huckle law works for and what does it not work for

  • works for low ionic strength / weak electrolytes

  • deviates at higher Ionic strength due to ‘excluded volume’

  • you’d need to modify the DH law to allow for

    • distance of closest approach → meaning it doesn’t account for the physical size of ions and treats them as point charges - as in the radius is 0

    • water of hydration bound to ions

    • ionic liquids - all conc electrolyte no solution

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what’s a room temperature ionic liquid

  • everything is an ion there is no solvent

  • they’re a liquid because the ions are large AND they don’t pack easily

  • have bad conductivity

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what are 3 types of metals

  1. conductors - band is not completely filled so it has accessible energy states for e-

  2. semi-conductors - band gap is comparable to thermal energy so at certain T , some e- are promotes

  3. insulators - band is full so no accessible states

<ol><li><p>conductors - band is not completely filled so it has accessible energy states for e- </p></li><li><p>semi-conductors - band gap is comparable to thermal energy so at certain T , some e- are promotes </p></li><li><p>insulators - band is full so no accessible states </p></li></ol><p></p>
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what is Fermi energy

  • the top of the valence band where all the interactions happen

  • it can be equated to chemical potential of the e- inside the solid

  • the energy of the e- can be changed by applying external electrical potential φ

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how does e- transfer work on orbitals and on the fermi energy

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electrochemical potential eq

φ = electrical potential (V)

μ— = electrochemical potential = +ve

<p>φ = electrical potential (V)</p><p><span>μ— = electrochemical potential = +ve</span></p>
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electrochemical potential eq of oxidised species

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overall electrochemical potential equation that shows the electrochemical potential of the reaction = 0

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equation where chemical potential eq is substituted in electrochemical potential eq

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electrode potential + nerst eq

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rearranged electrical potential equation that includes G

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daniel cell eq

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what does a Daniel cell look like

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how would you write the system of a cell

  • oxidation on the left

  • reduction on the right

<ul><li><p>oxidation on the left</p></li><li><p>reduction on the right</p></li></ul><p></p>
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what is the reference redox couple

  • the Hydrogen electrode (SHE)

<ul><li><p>the Hydrogen electrode (SHE)</p></li></ul><p></p>
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pH eq

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what does an ion selective electrode look like and what are the three phases

  • the 3 phases

    • analyte solution

    • reference solution

    • membrane

  • the target ion can go between all three

<ul><li><p>the 3 phases </p><ul><li><p>analyte solution </p></li><li><p>reference solution</p></li><li><p>membrane </p></li></ul></li><li><p>the target ion can go between all three </p></li></ul><p></p>
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electrochemical potential of analyte in an ion selective electrode eq

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ion transfer / electrical potential eq

  • tells us the electrical potential required to drag ions into the membrane phase

<ul><li><p>tells us the electrical potential required to drag ions into the membrane phase </p></li></ul><p></p>
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measured electrical potential difference eq

  • shows us that the difference in electrical potential between the two electrodes φref and φan is proportional to the ratio of activities of the distributing ion in the phases

<ul><li><p>shows us that the difference in electrical potential between the two electrodes <span>φref and φan is proportional to the ratio of activities of the distributing ion in the phases </span></p></li></ul><p></p>
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why store energy electrochemically?

  1. thermodynamic limit on efficiency of combustion energy → electrochemical has a higher limit

  2. greenhouse gas issues from combustion of hydrocarbons

  3. increasing use of renewable energy

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what are the 2 methods of storage of electrochemical energy

  1. reversible conversion of chemical energy → electrical energy - secondary battery

  2. irreversible conversion - primary battery ( can’t recharge)

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what are the disadvantages of batteries

  1. reactions not readily reversible - Zn2+ tends to form complexes that block contact between electrode and cathode

  2. MnO2 is a poor electrical conductor - need inert carbon to transfer e-

  3. heavy materials used - energy / mass ratio is low

  4. cell voltage is limited to 1.4 -1.7V

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what is the cathode and anode reaction on charging in non aqueous batteries

  • lithium batteries

  • the cathode and anode flip during discharging

<ul><li><p>lithium batteries </p></li><li><p>the cathode and anode flip during discharging </p></li></ul><p></p>
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energy density eq for batteries

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what are ideal battery characteristics

  1. max energy density

  2. reversibility

  3. safe, non-toxic

  4. light environments - use of Li

  5. not reactive in H2O

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what are disadvantages of Li batteries

  1. organic solvent required - flammable, toxic

  2. graphite intercalation used for prevention of formation of dendrites - dead weight

  3. use of transition metal oxides - expensive , heavy

  4. poor electrical conductivity

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what’s the graphical shape of charge and discharge of Li batteries

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what’s the problem with the Nernst eq

  • assumes equilibrium

  • sets a theoretical potential that can be achieved

  • we need to consider

    • kinetic loss

    • ohmic loss

    • conc loss