This document discusses voltaic cells and the potential differences between half-cells. It explains that connecting two half-cells with different electrode potentials through an external circuit and salt bridge allows electrons to flow spontaneously from the negative half-cell to the positive half-cell. Specifically, it gives the example of a Zn/Cu voltaic cell, where the Zn half-cell acts as the anode undergoing oxidation and the Cu half-cell acts as the cathode undergoing reduction. When connected, the potential difference between the half-cells can be measured as 1.10 volts using a high resistance voltmeter.
Class XII Electrochemistry - Nernst equation.Arunesh Gupta
Introduction, application of electrochemistry, metallic conduction & electrolytic conduction, electrolytes, electrochemical cell & electrolytic cell, Galvanic cell (Daniell cell), Standard reduction & oxidation potential, SHE as reference electrode, Standard emf of a cell or standard cell potential, Electrochemical series & its application, Nernst equation, Relationship between (i) Standard cell potential & equilibrium constant (ii) standard cell potential & standard Gibbs energy, some numerical problems.
Class XII Electrochemistry - Nernst equation.Arunesh Gupta
Introduction, application of electrochemistry, metallic conduction & electrolytic conduction, electrolytes, electrochemical cell & electrolytic cell, Galvanic cell (Daniell cell), Standard reduction & oxidation potential, SHE as reference electrode, Standard emf of a cell or standard cell potential, Electrochemical series & its application, Nernst equation, Relationship between (i) Standard cell potential & equilibrium constant (ii) standard cell potential & standard Gibbs energy, some numerical problems.
Includes a discussion of Voltaic and electrolytic cells, the Nernst equation and the relationship between electrochemical processes, chemical equilibrium and free energy.
**More good stuff available at:
www.wsautter.com
and
http://www.youtube.com/results?search_query=wnsautter&aq=f
Preparation and reaction of aldehyde and ketone, electromeric effect, aldol condensation, cannizarro reaction, perkin condensation, benzoin condensation, nucleophilic addition reaction and uses of aldehyde and ketone
a solution is a homogeneous mixture composed of two or more substances. In such a mixture, a solute is a substance dissolved in another substance, known as a solvent.
Includes a discussion of Voltaic and electrolytic cells, the Nernst equation and the relationship between electrochemical processes, chemical equilibrium and free energy.
**More good stuff available at:
www.wsautter.com
and
http://www.youtube.com/results?search_query=wnsautter&aq=f
Preparation and reaction of aldehyde and ketone, electromeric effect, aldol condensation, cannizarro reaction, perkin condensation, benzoin condensation, nucleophilic addition reaction and uses of aldehyde and ketone
a solution is a homogeneous mixture composed of two or more substances. In such a mixture, a solute is a substance dissolved in another substance, known as a solvent.
A tunnel diode or Esaki diode is a type of semiconductor that is capable of very fast operation, well into the microwave frequency region, made possible by the use of the quantum mechanical effect called tunneling.
It was invented in August 1957 by Leo Esaki when he was with Tokyo Tsushin Kogyo, now known as Sony. In 1973 he received the Nobel Prize in Physics, jointly with Brian Josephson, for discovering the electron tunneling effect used in these diodes. Robert Noyce independently came up with the idea of a tunnel diode while working for William Shockley, but was discouraged from pursuing it.[1]
These diodes have a heavily doped p–n junction only some 10 nm (100 Å) wide. The heavy doping results in a broken bandgap, where conduction band electron states on the n-side are more or less aligned with valence band hole states on the p-side
Tunnel diodes were first manufactured by Sony in 1957[2] followed by General Electric and other companies from about 1960, and are still made in low volume today.[3] Tunnel diodes are usually made from germanium, but can also be made from gallium arsenide and silicon materials. They are used in frequency converters and detectors.[4] They have negative differential resistance in part of their operating range, and therefore are also used as oscillators, amplifiers, and in switching circuits using hysteresis.
Figure 6: 8–12 GHz tunnel diode amplifier, circa 1970
In 1977, the Intelsat V satellite receiver used a microstrip tunnel diode amplifier (TDA) front-end in the 14 to 15.5 GHz band. Such amplifiers were considered state-of-the-art, with better performance at high frequencies than any transistor-based front end.[5]
The highest frequency room-temperature solid-state oscillators are based on the resonant-tunneling diode (RTD).[6]
There is another type of tunnel diode called a metal–insulator–metal (MIM) diode, but present application appears restricted to research environments due to inherent sensitivities.[7] There is also a metal–insulator–insulator–metal MIIM diode which has an additional insulator layer. The additional insulator layer allows "step tunneling" for precise diode control.[8]
This is an introductory lecture on electrical services in buildings. This module deals with basic terminologies and formulae covered in school level physics. This is a brief recapitulation.
Model Attribute Check Company Auto PropertyCeline George
In Odoo, the multi-company feature allows you to manage multiple companies within a single Odoo database instance. Each company can have its own configurations while still sharing common resources such as products, customers, and suppliers.
Macroeconomics- Movie Location
This will be used as part of your Personal Professional Portfolio once graded.
Objective:
Prepare a presentation or a paper using research, basic comparative analysis, data organization and application of economic information. You will make an informed assessment of an economic climate outside of the United States to accomplish an entertainment industry objective.
Synthetic Fiber Construction in lab .pptxPavel ( NSTU)
Synthetic fiber production is a fascinating and complex field that blends chemistry, engineering, and environmental science. By understanding these aspects, students can gain a comprehensive view of synthetic fiber production, its impact on society and the environment, and the potential for future innovations. Synthetic fibers play a crucial role in modern society, impacting various aspects of daily life, industry, and the environment. ynthetic fibers are integral to modern life, offering a range of benefits from cost-effectiveness and versatility to innovative applications and performance characteristics. While they pose environmental challenges, ongoing research and development aim to create more sustainable and eco-friendly alternatives. Understanding the importance of synthetic fibers helps in appreciating their role in the economy, industry, and daily life, while also emphasizing the need for sustainable practices and innovation.
June 3, 2024 Anti-Semitism Letter Sent to MIT President Kornbluth and MIT Cor...Levi Shapiro
Letter from the Congress of the United States regarding Anti-Semitism sent June 3rd to MIT President Sally Kornbluth, MIT Corp Chair, Mark Gorenberg
Dear Dr. Kornbluth and Mr. Gorenberg,
The US House of Representatives is deeply concerned by ongoing and pervasive acts of antisemitic
harassment and intimidation at the Massachusetts Institute of Technology (MIT). Failing to act decisively to ensure a safe learning environment for all students would be a grave dereliction of your responsibilities as President of MIT and Chair of the MIT Corporation.
This Congress will not stand idly by and allow an environment hostile to Jewish students to persist. The House believes that your institution is in violation of Title VI of the Civil Rights Act, and the inability or
unwillingness to rectify this violation through action requires accountability.
Postsecondary education is a unique opportunity for students to learn and have their ideas and beliefs challenged. However, universities receiving hundreds of millions of federal funds annually have denied
students that opportunity and have been hijacked to become venues for the promotion of terrorism, antisemitic harassment and intimidation, unlawful encampments, and in some cases, assaults and riots.
The House of Representatives will not countenance the use of federal funds to indoctrinate students into hateful, antisemitic, anti-American supporters of terrorism. Investigations into campus antisemitism by the Committee on Education and the Workforce and the Committee on Ways and Means have been expanded into a Congress-wide probe across all relevant jurisdictions to address this national crisis. The undersigned Committees will conduct oversight into the use of federal funds at MIT and its learning environment under authorities granted to each Committee.
• The Committee on Education and the Workforce has been investigating your institution since December 7, 2023. The Committee has broad jurisdiction over postsecondary education, including its compliance with Title VI of the Civil Rights Act, campus safety concerns over disruptions to the learning environment, and the awarding of federal student aid under the Higher Education Act.
• The Committee on Oversight and Accountability is investigating the sources of funding and other support flowing to groups espousing pro-Hamas propaganda and engaged in antisemitic harassment and intimidation of students. The Committee on Oversight and Accountability is the principal oversight committee of the US House of Representatives and has broad authority to investigate “any matter” at “any time” under House Rule X.
• The Committee on Ways and Means has been investigating several universities since November 15, 2023, when the Committee held a hearing entitled From Ivory Towers to Dark Corners: Investigating the Nexus Between Antisemitism, Tax-Exempt Universities, and Terror Financing. The Committee followed the hearing with letters to those institutions on January 10, 202
How to Make a Field invisible in Odoo 17Celine George
It is possible to hide or invisible some fields in odoo. Commonly using “invisible” attribute in the field definition to invisible the fields. This slide will show how to make a field invisible in odoo 17.
Home assignment II on Spectroscopy 2024 Answers.pdf
IB Chemistry on Voltaic Cell, Standard Electrode Potential and Standard Hydrogen Electrode
1. Types voltaic cell
Conversion electrical energy
to chemical energy
Electrochemistry
Electrolytic cellVoltaic cell
NH4CI and ZnCI2
Chemical and electrical energy
Redox rxn
(Oxidation/reduction)
Movement electron
Produce electricity
Conversion chemical energy
to electrical energy
Electrodes– different metal (Half cell) Electrodes – same metal (Half cell)
Chemical
rxn
Electric current
Daniell cell Alkaline cellDry cell Nickel cadmium cell
Primary cell (Non rechargeable)
MnO2 and KOH
Secondary cell (Rechargeable)
2. Conversion electrical to chemical energy
Electrochemistry
ElectrolyticcellVoltaic cell
Conversion chemicalto electricalenergy
Cathode (+ve) - Reduction Cathode (-ve) - Reduction
Vs
Electron flow from anode (-ve) to cathode (+ve) electrode Electron flow from anode (+ve) to cathode (-ve) electrode
Anode
(-ve)
Spontaneous rxn Non Spontaneous rxn
Anode (-ve) – Oxidation Anode (+ve) – Oxidation
++
О
О
О
О
- -
Zn → Zn 2+ + 2e
(oxidized)
Cu2+ + 2e → Cu
(reduced)
Zn2+
Zn2+
Zn2+
Zn2+-
-
-
-
→ +
+
+
Cu2+
Cu2+
Cu2+
-e
-e
+
+
+ -
-
-
X-→ X + -e
(oxidized)
X
-
X
-
X
-
Anode
(+ve)
Cathode
(-ve)
Cathode
(+ve)
-e
-e
Y+ + e- → Y
(reduced)
Y+
Y+
Y+
-e
-e
-e
-e
Anode Cathode
Voltaic Cell Electrolytic Cell
Anode Oxidation Negative (-ve) Oxidation Positive (+ve)
Cathode Reduction Positive (+ve) Reduction Negative (-ve)
Cation (+ve ion) to cathode (-ve)Anion (-ve ion) to anode (+ve)
3. Current– measured in Amperes or Coulombs per second
1A = 1 Coulomb charge pass througha point in 1 second = 1C/s
1 Coulomb charge (electron)= 6.28 x 10 18 electronspassing in 1 second
1 electron/protoncarry charge of – 1.6 x 10 -19 C ( very small)
6.28 x 10 18 electron carry charge of - 1 C
Electric current
Flow electric charges (electron, -ve)
From High electric potential – low potential
Due to Potential Difference– measure with ammeter
ond
electron
ond
Coulomb
A
sec.1
.1028.6
sec1
1
1
18
Click here current/voltage
Current Electric Current – movingcharges in solid wire or solution
Flow of
charges
-
-
-
Solid/WireSolution/Electrolyte
Electron move in random
No current flow cause
No potential difference
Electrons & Protons
-
-
+
+
1A = 6.28 x 1018 e
1 second
Video on current/voltage
Potential Difference across wire
Electron move in one direction
Current flow
+ve ions -ve ions
(cations) (anions)
Potential Difference applied/Battery used
ItQ t = Time/ s
Find amt charges pass through a sol if
Current is 2.ooA, time is 15 mins
ItQ
Current flow
Q = Amt Charges/ C I = Current/ A
CQ 1800601500.2
4. Electric Potential
C
J
Volt
1
1
Potential Diff/Voltage
-Measured in Volt with Voltmeter
- 1 V = 1 Joule energy released when 1 Coulomb
charge pass through 1 point
- 1 V = 1 J/C
6V battery - 6J energy for every Coulomb
moved bet its terminals.
V = Potential Diff
I = Current
R = Resistance
Potential diff bet 2 points is 1 V
↓
1 J energy released when 1 C charge passes through
Voltmeter across
1Volt
1 V
Potential Diff/Voltage/PotentialEnergy
+ -
1 Ω 2 Ω
Charges (-ve)
flow down
A
R
V
I
RIV
2
3
6
VV
RIV
212
-
+
-
+
VV
RIV
422
Total current
Potential Diff(PD)vs Current
PD = Water Pressure
PD = 1.5V – 1.5J energy released 1C charge flow down
PD – cause charge flow- charge flow = Called CURRENT
Potential Diff(PD)vs Current
1.5V = 1.5J/C
A
DElectric potential/PD/Voltage = Electric Pressure = Volt
Electric Current/Current = Charge flow = Amp
Electric Potential Energy = Work done to bring a charge to a point = Joule
Voltage NOT same as energy, Voltage = energy/charge
Battery lift charges, Q to higher potential
Potential Energy bet 2 terminals in battery stored as chemical energy
2A 2A
5. EMF vs PD
V = Potential Diff
I = Current
R = Resistance
Max potential diff bet two
electrodes of battery source.
+ -
1 Ω 2 Ω
A
R
V
I
RIV
2
3
6
VV
RIV
212
VV
RIV
422
Total current
Current flow Circuit complete
Circuit complete
↓
Current flow
↓
Internal resistance
(battery - 1Ω)
↓
Terminal PD = 8V
(Voltage drop)
Potential Diff/Voltage in Volt
Symbol for EMF = E or ℰ
Click here voltage drop
internal resistance
No Current flow in circuit
EMF (ElectromotiveForce) in Volt
Battery = EMF = 9V
9 Volt
).(9 currentnoVEMFV
IRV
EMF Internal resistance Ir
Place voltmeter across – EMF= 9V
No current flow.
A
rR
E
I
rRIE
IrIREMFE
1
9
9
)18(
9
)(
)(
)(
VV
RIV
881
VV
RIV
111
EMF = 8V+1V
8 Volt
1 Volt
Voltage measured across terminal = 8V Click here EMF notes Click here PD, PE and I
EMF (6V) = 2V + 4V
4 Volt2 Volt
Charges passing through wire
Current flow Circuit complete
6. Series vs Parallel Circuit
3 Ω
A
R
V
I
RIV
5.0
18
9
VV
V
RIV
5.2
55.0
VV
V
RIV
5
105.0
Total Resistance
3 + 10 + 5 = 18Ω
Parallel CircuitSeries Circuit
EMF (9V) = 2.5V + 5V + 1.5V
R = 0.625Ω
Voltage same across all component. VT = V1 = V2 = V3
Total current = sum of current in each branch. IT = I1 + I2 + I3
Total equi resistance < value of any individual resistor
Total Current
Current same in circuit
Total voltage = sum of component in series
5 Ω
10 Ω0.5 A
VV
V
RIV
5.1
35.0
Voltage across all component
Same = 9V
Total Current = sum of all current in each branch
Total Resistance
10Ω 2Ω 1Ω
AI
R
V
I
9.0
10
9
AI
R
V
I
5.4
2
9
AI
R
V
I
9
1
9
Total current (14.4A) = 0.9A + 4.5A + 9A
Ohm’s Law
Sum voltage drop equal to voltage source (EMF). VT = V1 + V2 + V3
Current same in all components in series.
Total resistance = sum of individual resistances. RT = R1 + R2 + R3
Click here voltage drop
Series Circuit Parallel Circuit
• Voltage do not flow
• Charges/Current flow
• Voltage cause current to flow
• Voltage ≠ Energy
• Battery do not supply electron
• Wire contain electron, they flow
Electron in wire repel by -ve terminal move in circuit
Electron move slowly, drift velocity, electric field move at speed of light
Electric signal travel speed of light, bulb light up instantaneously,
Electric signal/field travel faster than movement of electron
Movement e – cause electric field – travel speed of light – bulb light up
Voltage Diff – Pressure diff across
Voltage Diff – Cause water/current to flow
14.4A 4.5A0.9A 9A
7. Potential Diff bet Zn/Zn2+
Electrode potential Zn/Zn2+ = -ve
-
Electrode Potential
Redox Equilibrium
Zn2+
Zn → Zn 2+ + 2e
(Oxidation)
Zn 2+ + 2e → Zn
(Reduction)
Zn 2+ + 2e ↔ Zn
(At equilibrium)
Metal Zn placed in its sol Zn2+ ion
Equilibrium bet Zn/Zn2+
Zn metal reactive lose e form Zn2+
Equilibrium shift to right ←
Potential Diff form bet Zn/Zn2+
Potential Diff
Electrode potential = -ve
Zn2+
Zn2+
Zn
Zn2+
Zn
Zn2+
Zn2+ Zn2+
Zn 2+ + 2e ↔ Zn
Equi shift to ←
-
--
Zn
-
-
-
-
+
+
+
+
+ +
+ +
+
Voltage of Zn/Zn2+ can’t be measured.
Abs electrodepotentialcan’t measured.
Only Diff in electrode potentialcan be measured.
Cannot measure
Abs Potential
Metal Cu placed in its sol Cu2+ ion
Equilibrium bet Cu/Cu2+
Cu2+ ion gain -2e form Cu
Equilibrium shift to left ←
Potential Diff form bet Cu/Cu2+
Potential Diff
Electrode potential = +ve
Cu
Cu2+
Cu2+
Cu2+
Cu2+
Cu → Cu2+ + 2e
(Oxidation)
Cu2+ + 2e → Cu
(Reduction)
Cu2+ + 2e ↔ Cu
(At equilibrium)
Cu
-e
-e
-e
Cu2+
Cu2+
Cu2+
Cu2+ + 2e ↔ Cu
Equi shift to →
Zn Half Cell
+
+
+
Cu
+
+
+
---
-
--- ----
--
Potential Diff bet Cu/Cu2+
Electrode potential Cu/Cu2+ = +ve
Cannot measure
Abs Potential
Voltage of Cu/Cu2+can’t be measured.
Abs electrodepotentialcan’t measured.
Only Diff in electrode potentialcan be measured.
Click here chem database
(std electrode potential)
Click here chem database
(std electrode potential)
Click here interactive ECS Click here pdf version ECS
Cu Half Cell
8. PotentialDiff Cu/Cu2+
Electrode potential
Cu/Cu2+ = +ve
PotentialDiff Zn/Zn2+
Electrode potential
Zn/Zn2+ = -ve
Zn2+
Zn → Zn 2+ + 2e
(Oxidation)
Zn 2+ + 2e → Zn
(Reduction)
Zn 2+ + 2e ↔ Zn
(At equilibrium)
Zn2+
Zn2+
Zn
Zn2+
Zn
Zn2+
Zn2+ Zn2+
Zn 2+ + 2e ↔ Zn
Equi shift to ←
-
-
-
Zn
-
--
-
+
++
+
+ +
+
+
+
Can’t measure
Abs Potential
Cu
Cu2+
Cu2+
Cu2+
Cu2+
Cu → Cu2+ + 2e
(Oxidation)
Cu2+ + 2e → Cu
(Reduction)
Cu2+ + 2e ↔ Cu
(At equilibrium)
Cu
-e
-e
-e
Cu2+
Cu2+
Cu2+
Cu2+ + 2e ↔ Cu
Equi shift to →
Zn Half Cell
+
+
+
Cu
+
+
+
-
Cu Half Cell
Zn/Cu Voltaic Cell
External circuit – flow of electrons
Complete circuit
-
--
--
-
-
----
-- -
Connect 2 Half Cell with wire/ salt bridge
Zn half cell (-ve)
Oxidation
Cu half cell (+ve)
Reduction
Salt Bridge – flow of ions
Complete the circuit
Cu2+ + 2e → CuZn → Zn 2+ + 2e
Zn + Cu2+ → Zn2+ + Cu
Anode Cathode
Maintain electrical
neutrality
Salt bridge – saturated KNO3
Zn2+ increase ↑
NO3
- flow in to balance excess Zn2+
Cu2+ decrease ↓, excess –ve ion ↑
K+ flow in to balance loss of Cu2+
Zn Cu
--
-
-
Zn2+
Zn2+
Zn2+
Excess of Zn2+ ion
+
+
++
-
-
-
-
---
-
-
-
-
-
Excess of –ve ion
+
+
+
+
++
+
Without Salt Bridge
-+
+
+
+
With Salt Bridge
(electron unable to flow due to ESF)
NO3
-
NO3
-
NO3
-
NO3
-
+
+
+ K
+
K
+
K
+
-
-
-
K+ flow in to balance
excess of – ion
NO3
-
flow in to balance
excess of + ion
2 Half Cell to make a Voltaic Cell
-e -e
-
-
-
-
+
+
+
+
9. PotentialDiff Cu/Cu2+
Electrode potential
Cu/Cu2+ = +ve
PotentialDiff Zn/Zn2+
Electrode potential
Zn/Zn2+ = -ve
Zn2+
Zn → Zn 2+ + 2e
(Oxidation)
Zn 2+ + 2e → Zn
(Reduction)
Zn 2+ + 2e ↔ Zn
(At equilibrium)
Zn2+
Zn2+
Zn
Zn2+
Zn
Zn2+
Zn2+ Zn2+
Zn 2+ + 2e ↔ Zn
Equi shift to ←
-
-
-
Zn
-
--
-
+
++
+
+ +
+
+
+
Can’t measure
Abs Potential
Cu
Cu2+
Cu2+
Cu2+
Cu2+
Cu → Cu2+ + 2e
(Oxidation)
Cu2+ + 2e → Cu
(Reduction)
Cu2+ + 2e ↔ Cu
(At equilibrium)
Cu
-e
-e
-e
Cu2+
Cu2+
Cu2+
Cu2+ + 2e ↔ Cu
Equi shift to →
+
+
+
Cu
+
+
+
-
External circuit – flow of electrons
Complete circuit
-
--
--
-
-
----
-- -
Connect 2 Half Cell with wire/ salt bridge
Zn half cell (-ve)
Oxidation
Cu half cell (+ve)
Reduction
Voltmeter – High resistance
(No current flow) Salt Bridge – flow of ions
Complete the circuit
Cu2+ + 2e → CuZn → Zn 2+ + 2e
1.10Volt
Potential diff can be measured.
Voltmeter across – EMF
1.10 Volt
Zn + Cu2+ → Zn2+ + Cu
Anode Cathode
Zn(s) | Zn2+
(aq) || Cu2+
(aq)| Cu (s)
Cell diagram
Anode Cathode
Half Cell Half Cell
(Oxidation) (Reduction)
Phase boundarySalt Bridge Flow
electrons
Maintain electrical
neutrality
Salt bridge – saturated KNO3
Zn2+ increase ↑
NO3
- flow in to balance excess Zn2+
Cu2+ decrease ↓
K+ flow in to balance loss of Cu2+
Zn/Cu Voltaic Cell 2 Half Cell to make a Voltaic Cell
Zn Half Cell Cu Half Cell
-e -e
-
-
-
-
+
+
+
+
10. PotentialDiff Ag/Ag2+
Electrode potential
Ag/Ag2+ = +ve
PotentialDiff Zn/Zn2+
Electrode potential
Zn/Zn2+ = -ve
Zn2+
Zn → Zn 2+ + 2e
(Oxidation)
Zn 2+ + 2e → Zn
(Reduction)
Zn 2+ + 2e ↔ Zn
(At equilibrium)
Zn2+
Zn2+
Zn
Zn2+
Zn
Zn2+
Zn2+ Zn2+
Zn 2+ + 2e ↔ Zn
Equi shift to ←
-
-
-
Zn
-
--
-
+
++
+
+ +
+
+
+
Can’t measure
Abs Potential
Ag
Ag+
Ag+
Ag+
Ag+
Ag → Ag+ + e
(Oxidation)
Ag+ + e → Ag
(Reduction)
Ag+ + e ↔ Ag
(At equilibrium)
Ag
-e
-e
-e
Ag+
Ag+
Ag+
Ag+ + e ↔ Ag
Equi shift to →
+
+
+
Ag
+
+
+
-
External circuit – flow of electrons
Complete circuit
-
--
--
-
-
----
-- -
Connect 2 Half Cell with wire/ salt bridge
Zn half cell (-ve)
Oxidation
Ag half cell (+ve)
Reduction
Voltmeter – High resistance
(No current flow) Salt Bridge – flow of ions
Complete the circuit
Ag+ + e → AgZn → Zn 2+ + 2e
1.56Volt
Potential diff can be measured.
Voltmeter across – EMF
1.56 Volt
Zn + 2Ag+ → Zn2+ + 2Ag
Anode Cathode
Zn(s) | Zn2+
(aq) || Ag+
(aq)| Ag (s)
Cell diagram
Anode Cathode
Half Cell Half Cell
(Oxidation) (Reduction)
Phase boundarySalt Bridge Flow
electrons
Maintain electrical
neutrality
Salt bridge – saturated KNO3
Zn2+ increase ↑
NO3
- flow in to balance excess Zn2+
Ag+ decrease ↓
K+ flow in to balance loss of Ag+
Zn/Ag Voltaic Cell 2 Half Cell to make a Voltaic Cell
Zn Half Cell Ag Half Cell
Ag
Ag+
-e -e
-
-
-
-
+
+
+
+
11. PotentialDiff Ag/Ag2+
Electrode potential
Ag/Ag2+ = +ve
PotentialDiff Cu/Cu2+
Electrode potential
Cu/Cu2+ = -ve
Cu2+
Cu → Cu 2+ + 2e
(Oxidation)
Cu 2+ + 2e → Cu
(Reduction)
Cu 2+ + 2e ↔ Cu
(At equilibrium)
Cu2+
Cu2+
Cu
Cu2+
Cu
Cu2+
Cu2+ Cu2+
Cu 2+ + 2e ↔ Cu
Equi shift to ←
-
-
-
Cu
-
--
-
+
++
+
+ +
+
+
+
Can’t measure
Abs Potential
Ag
Ag+
Ag+
Ag+
Ag+
Ag → Ag+ + e
(Oxidation)
Ag+ + e → Ag
(Reduction)
Ag+ + e ↔ Ag
(At equilibrium)
Ag
-e
-e
-e
Ag+
Ag+
Ag+
Ag+ + e ↔ Ag
Equi shift to →
+
+
+
Ag
+
+
+
-
External circuit – flow of electrons
Complete circuit
-
--
--
-
-
----
-- -
Connect 2 Half Cell with wire/ salt bridge
Cu half cell (-ve)
Oxidation
Ag half cell (+ve)
Reduction
Voltmeter – High resistance
(No current flow) Salt Bridge – flow of ions
Complete the circuit
Ag+ + e → AgCu → Cu 2+ + 2e
0.46Volt
Potential diff can be measured.
Voltmeter across – EMF
0.46 Volt
Cu + 2Ag+ → Cu2+ + 2Ag
Anode Cathode
Cu(s) | Cu2+
(aq) || Ag+
(aq)| Ag (s)
Cell diagram
Anode Cathode
Half Cell Half Cell
(Oxidation) (Reduction)
Phase boundarySalt Bridge Flow
electrons
Maintain electrical
neutrality
Salt bridge – saturated KNO3
Cu2+ increase ↑
NO3
- flow in to balance excess Cu2+
Ag+ decrease ↓
K+ flow in to balance loss of Ag+
Cu/Ag Voltaic Cell 2 Half Cell to make a Voltaic Cell
Cu Half Cell Ag Half Cell
Ag
Ag+
Cu
Cu2+
-e -e
-
-
-
-
+
+
+
+
12. Standard Electrode Potential
Standard HydrogenElectrode (SHE)
Platinum coat with Platinum oxide/black
– increase surface area for adsorption H2
- catalyze equilibrium bet H2 /H+
- H2 ↔ 2H+ + 2e-
Eθ
Standard Reference electrode
All Cell Potential are measured against
• Conc ( 1M)
• Pressure (1 atm)
• Temp (298K)
• Platinum-inert electrode
(sys without metal)
Standard
condition
H2 at 1 atm
Platinum
H2 gas
Pt wire
Platinum
2H+ + 2e ↔ H2
Eθ
= 0V
Types of Half Cells
Metal/ Ion (M/M+)
Gas/ Ion (M/M-)
Ion/ Ion (Fe3+/Fe2+)
• Pure Zn metal
• Conc (1M Zn2+)
• Pressure (1 atm)
• Temp(298K)
Condition Std Zn/Zn2+
Condition Std CI2/CI-
• CI2 gas
• Platinum electrode
• Conc (1M CI-)
• Pressure (1 atm)
• Temp(298K)
• Platinum electrode
• Conc (1M Fe3+/Fe2+)
• Pressure (1 atm)
• Temp(298K)
Condition Std Fe3+/ Fe2+
Zn2+
Zn
Fe3+/Fe2+
CI-
Condition for Standard
C
A
N
T
M
E
A
S
U
R
E
A
B
S
P
O
T
E
N
T
I
A
L
1
2
3
How to measure
electrode
potential ?
Pt
1M H+
Measure
Difference?
13. Standard Electrode Potential
Std HydrogenElectrode (SHE)
Eθ
= 0V
Types of Half Cells
Metal/ Ion (M/M+)
Gas/ Ion (M/M+)
Ion/ Ion (Fe3+/Fe2+)
• Pure Zn metal
• Conc (1M Zn2+)
• Pressure (1 atm)
• Temp(298K)
Condition Std Zn/Zn2+
Condition Std CI2/CI-
• CI2 gas
• Platinum electrode
• Conc (1M CI-)
• Pressure (1 atm)
• Temp(298K)
• Platinum electrode
• Conc (1M Fe3+/Fe2+)
• Pressure (1 atm)
• Temp(298K)
Condition Std Fe3+/ Fe2+
Zn2+
Zn
Fe3+/Fe2+
1
2
3
Connect to SHE
Connect to SHE
Connect to SHE
Eθ
= 0V
Eθ
= 0V
Eθ
= -0.76V
Standard electrode potential Zn/Zn2+ = -0.76V
Eθ
cell = -0.76V
Eθ
= +0.77V
Eθ
= +1.35V
Standard electrode potential Fe3+/Fe2+ = +0.77V
Eθ
cell = +0.77V
Standard electrode potential CI2 /CI- = +1.35V
Eθ
cell = +1.35V
Eθ
= -0.76V
Eθ
= +0.77V
Eθ
= +1.35V
2 Half Cellwith SHE as referenceelectrode
CI-
Pt
+
+
+
Pt
14. Standard Electrode Potential
Std Electrode Potential diff systems
Eθ
= 0V
Eθ
= 0V
Eθ
= 0V
Eθ
= -0.76V
Standard electrode potential Zn/Zn2+ = -0.76V
Eθ
cell = -0.76V
Eθ
= +0.77V
Eθ
= +1.35V
Standard electrode potential Fe3+/Fe2+ = +0.77V
Eθ
cell = +0.77V
Standard electrode potential CI2 /CI- = +1.35V
Eθ
cell = +1.35V
Eθ
= -0.76V
Eθ
= +0.77V
Eθ
= +1.35V
STANDARD Reduction potential – Hydrogen as std
Oxidized sp ↔ Reduced sp Eθ/V
Li+ + e- ↔ Li -3.04
K+ + e- ↔ K -2.93
Ca2+ + 2e- ↔ Ca -2.87
Na+ + e- ↔ Na -2.71
Mg 2+ + 2e- ↔ Mg -2.37
Al3+ + 3e- ↔ AI -1.66
Mn2+ + 2e- ↔ Mn -1.19
H2O + e- ↔ 1/2H2 + OH- -0.83
Zn2+ + 2e- ↔ Zn -0.76
Fe2+ + 2e- ↔ Fe -0.45
Ni2+ + 2e- ↔ Ni -0.26
Sn2+ + 2e- ↔ Sn -0.14
Pb2+ + 2e- ↔ Pb -0.13
H+ + e- ↔ 1/2H2 0.00
Cu2+ + e- ↔ Cu+ +0.15
SO4
2-
+ 4H+ + 2e- ↔ H2SO3 + H2O +0.17
Cu2+ + 2e- ↔ Cu +0.34
1/2O2 + H2O +2e- ↔ 2OH- +0.40
Cu+ + e- ↔ Cu +0.52
1/2I2 + e- ↔ I- +0.54
Fe3+ + e- ↔ Fe2+ +0.77
Ag+ + e- ↔ Ag +0.80
1/2Br2 + e- ↔ Br- +1.07
1/2O2 + 2H+ +2e- ↔ H2O +1.23
Cr2O7
2-+14H+ +6e- ↔ 2Cr3+ + 7H2O +1.33
1/2CI2 + e- ↔ CI- +1.35
MnO4
-
+ 8H+ + 5e- ↔ Mn2+ + 4H2O +1.51
1/2F2 + e- ↔ F +2.87
-ve
reduction
potential
+ve
reduction
potential
Click here std analogy video
Click here std analogy
Click here chem database
(std electrode potential)
Compared to
H2 as std
Eθ
cell/CellPotential= EMF in volt
EMF prod when half cell connect to SHE at std condition
Std electrode potential written as std reduction potential
29. Standard Electrode Potential
STANDARD Reduction potential – H2 as std
Oxidized sp ↔ Reduced sp Eθ/V
Li+ + e- ↔ Li -3.04
K+ + e- ↔ K -2.93
Ca2+ + 2e- ↔ Ca -2.87
Na+ + e- ↔ Na -2.71
Mg 2+ + 2e- ↔ Mg -2.37
Al3+ + 3e- ↔ AI -1.66
Mn2+ + 2e- ↔ Mn -1.19
H2O + e- ↔ H2+OH- -0.83
Zn2+ + 2e- ↔ Zn -0.76
Fe2+ + 2e- ↔ Fe -0.45
Ni2+ + 2e- ↔ Ni -0.26
Sn2+ + 2e- ↔ Sn -0.14
Pb2+ + 2e- ↔ Pb -0.13
H+ + e- ↔ 1/2H2 0.00
Cu2+ + e- ↔ Cu+ +0.15
SO4
2-
+ 4H+ + 2e- ↔ H2SO3 + H2O +0.17
Cu2+ + 2e- ↔ Cu +0.34
1/2O2 + H2O +2e- ↔ 2OH- +0.40
Cu+ + e- ↔ Cu +0.52
1/2I2 + e- ↔ I- +0.54
Fe3+ + e- ↔ Fe2+ +0.77
Ag+ + e- ↔ Ag +0.80
1/2Br2 + e- ↔ Br- +1.07
1/2O2 + 2H+ +2e- ↔ H2O +1.23
Cr2O7
2-+14H+ +6e- ↔ 2Cr3+ +7H2O +1.33
1/2CI2 + e- ↔ CI- +1.36
MnO4
-
+ 8H+ + 5e- ↔ Mn2+ + 4H2O +1.51
1/2F2 + e- ↔ F +2.87
-ve
reduction
potential
+ve
reduction
potential
Compared to
H2 as std
Eθ
cell/CellPotential= EMF in volt
EMF when half cell connect to SHE std condition
Std potentialwritten as std reduction potential
TOP right
• High ↑ tendency lose e
• Li → Li +
+ e
• Eθ
Li = +3.04V
• STRONG reducingAgent
•Oxi favourable (Eθ =+ve)
STRONG
Reducing Agent
WEAK
Reducing Agent
BOTTOM right
• Low ↓ tendency lose e
• F - → 1/2F2 + e
• Eθ
F2 = - 2.87V
• WEAK reducingAgent
•Oxi NOT favourable (Eθ =-ve)
WEAK
Oxidizing Agent
Strong
Oxidizing Agent
TOP left
• Low ↓ tendency gain e
• Li+
+ e → Li
• Eθ
Li= - 3.04V
• WEAK oxidizingAgent
• Red NOT favourable
(Eθ =-ve)
BOTTOM left
• High ↑ tendency gain e
• F2 + 2e → 2F-
• Eθ
F2= +2.87V
• STRONG oxidizing Agent
•Red favourable
(Eθ =+ve)
30. Acknowledgements
Thanks to source of pictures and video used in this presentation
Thanks to Creative Commons for excellent contribution on licenses
http://creativecommons.org/licenses/
http://spmchemistry.onlinetuition.com.my/2013/10/electrolytic-cell.html
http://www.chemguide.co.uk/physical/redoxeqia/introduction.html
http://educationia.tk/reduction-potential-table
http://2012books.lardbucket.org/books/principles-of-general-chemistry-v1.0/s23-
electrochemistry.html
Prepared by Lawrence Kok
Check out more video tutorials from my site and hope you enjoy this tutorial
http://lawrencekok.blogspot.com