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THERMODYNAMICS
Presentation by
Dr. Satyajit Mandal
What is thermodynamics ?
 The science of energy, that
concerned with the ways in which
energy is stored within a body.
 Energy transformations -mostly
involve heat and work
movements.
 The Fundamental law is the
conservation of energy principle:
energy cannot be created or
destroyed, but can only be
transformed from one form to
another.
2
System, surroundings and boundary
 System: A quantity of matter or a
region in space chosen for study.
 Surroundings: The mass or region
outside the system
 Boundary: The real or imaginary
surface that separates the system
from its surroundings.
3
Type of system
Open system
 Open system – both
mass and energy can
cross the selected
boundary.
 Example: an open cup
of coffee
4
Type of system
Closed system
 Closed system – only
energy can cross the
selected boundary.
 Examples: a tightly
capped cup of coffee.
5
Type of system
Isolated system
 Isolated system –
neither mass nor
energy can cross the
selected boundary.
 Example: coffee in a
closed, well-insulated
thermos-bottle
Thermally insulated wall.
6
Properties of a system
7
Properties of a system
8
State, Equilibrium and Process
State – a set of properties that
describes the conditions of a system.
Eg. Mass m, Temperature T, volume V.
Thermodynamic equilibrium
system that maintains thermal,
mechanical, phase and chemical
equilibriums.
9
State, Equilibrium and Process
Process – change from one state to another state.
Process Property held constant
1. isobaric pressure
2. isothermal temperature
3. isochoric volume
4.isentropic entropy
5.Polytropic heat capacity
10
State, Equilibrium and Process
The prefix “iso”- is often used to designate a process for which a particular property
remains constant.
Isobaric process: A process during which the pressure P remains constant. Pressure is
Constant (ΔP = 0)
Isobaric process:
11
State, Equilibrium and Process
Isochoric (or isometric) process: A process during which the specific volume V
remains constant.
Isochoric process:
Isothermal process: A process during
which the temperature T remains
constant.
Isothermal process:
12
State, Equilibrium and Process
Cyclic process - when a system in a given initial
state goes through various processes and finally
return to its initial state, the system has undergone
a cyclic process or cycle.
Reversible process – system can restored to it’s initial state
from final state without the aid of any external agency.
Irreversible process – once the final state reached, system
can not reverse back to its initial state without the aid of
external agency.
Adiabatic process - a process that has no heat transfer
into or out of the system. It can be considered to be
perfectly insulated.
13
Explanation of reversible process
Reversible process
14
Key features of reversible process:
• Driving and opposing force differ by infinitesimal
amount.
• Process occurs at very slowly & take infinite time to
complete.
• At every step, system attains equilibrium.
• Most of the natural process are irreversible except
phase changes ( melting/freezing of ice/water at 0°C
& 1 atm pressure.
Path function and state function
15
Zeroth Law of Thermodynamics
“ If two bodies are in thermal equilibrium with a third body, there are also in thermal
equilibrium with each other.”
16
WORK
17
WORK
18
Work done in reversible process for an ideal gas:
First law of thermodynamics and internal energy
The first law of thermodynamics states that the amount of heat given to a
system is equal to the sum increase in the internal energy of the system and the
external work done.
Statement of the first law of thermodynamics
 Conservation of energy.
 Energy can neither be created nor destroyed but it can change forms.
 Total amount of energy in a closed system remains constant.
Description with formula
Heat/work formula:
ΔU=Q-W
dU= ΔQ-PdV
(W=PdV)
19
Significance and limitation
Significance:
 The total amount of energy in the world is constant.
 It is impossible to get more energy out of a system than is put into it.
 You can’t get energy from nothing.
Limitation:
First law does not help to predict whether the certain process is possible or not.
Reason:
It does not specify that heat cannot flow from low temperature body to a high temperature
body.
20
Enthalpy(H) and Heat capacity (Cp & Cv)
21
Enthalpy:
A thermodynamic quantity equivalent to the total heat content of a system is called enthalpy.
Denoted by ‘H’.
H=U+PV; where U is internal energy, P & V are pressure and temperature.
Change in enthalpy;
ΔH=ΔU+ΔPV
ΔH = ΔU+PΔV+VΔP; at constant pressure, ΔH= ΔU+PΔV
Classification of reactions based on ΔH
Exothermic reactions (ΔH = (-) ve) (HCl+NaOH NaCl +H2O+heat)
An exothermic reaction is a reaction that releases energy to the surroundings.
2. Endothermic reactions (ΔH = (+)ve) ;(N2(g)+O2(g) +heat 2NO (g))
An endothermic reaction is a reaction that absorbs energy from the surroundings.
Enthalpy(H) and Heat capacity (Cp & Cv)
22
Heat Capacity:
It is the amount of heat required to increase the temperature by 1° C.
q = cΔT; the coefficient c is called heat capacity.
Specific Heat Capacity:
The amount of energy needed to increase the temperature of 1 gram of a material by 1 °C is
known as its specific heat.
q = m csΔT; q is heat, m is mass, ΔT is change in temperature, the coefficient cs is called
specific heat capacity.
CP and CV Specific heat capacity at constant pressure and constant volume.
Relation between Cp and Cv:
qP = nCP∆T = ∆H (1); qV = nCV∆T = ∆U (2)
∆H = ∆U + ∆(pV ) = ∆U + ∆(RT) = ∆U + R ∆T (for 1 mole ideal gas; PV=RT)
∆H = ∆U + R ∆T (3)
Using the equn. 1&2 in 3,
we get ; CP∆T = CV∆T + R ∆T
CP –CV =R
CP/CV =γ; γ is 1.6, 1.4 and 1.3 for mono, di and polyatomic gases.
Standard Enthalpy(H⦵) and Thermochemistry
23
Various enthalpy changes:
1. Standard enthalpy change of reaction, ΔH° r (in general)
2. Standard enthalpy change of formation, ΔH°f
3. Standard enthalpy change of combustion, ΔH°c
4. Standard enthalpy change of neutralisation, ΔH°n
5. Standard enthalpy change of atomisation, ΔH°at
6. Standard enthalpy change of solution, ΔH°sol
7. Standard enthalpy change of hydration, ΔH°hyd
Standard condition: Temparature298K and Pressure1 atm (~100 Kpa)
Common interpretation:
Enthalpy change of 1 mole substance  due to some physical process.

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Thermodynamics-lecture-notes-part1.pptx

  • 2. What is thermodynamics ?  The science of energy, that concerned with the ways in which energy is stored within a body.  Energy transformations -mostly involve heat and work movements.  The Fundamental law is the conservation of energy principle: energy cannot be created or destroyed, but can only be transformed from one form to another. 2
  • 3. System, surroundings and boundary  System: A quantity of matter or a region in space chosen for study.  Surroundings: The mass or region outside the system  Boundary: The real or imaginary surface that separates the system from its surroundings. 3
  • 4. Type of system Open system  Open system – both mass and energy can cross the selected boundary.  Example: an open cup of coffee 4
  • 5. Type of system Closed system  Closed system – only energy can cross the selected boundary.  Examples: a tightly capped cup of coffee. 5
  • 6. Type of system Isolated system  Isolated system – neither mass nor energy can cross the selected boundary.  Example: coffee in a closed, well-insulated thermos-bottle Thermally insulated wall. 6
  • 7. Properties of a system 7
  • 8. Properties of a system 8
  • 9. State, Equilibrium and Process State – a set of properties that describes the conditions of a system. Eg. Mass m, Temperature T, volume V. Thermodynamic equilibrium system that maintains thermal, mechanical, phase and chemical equilibriums. 9
  • 10. State, Equilibrium and Process Process – change from one state to another state. Process Property held constant 1. isobaric pressure 2. isothermal temperature 3. isochoric volume 4.isentropic entropy 5.Polytropic heat capacity 10
  • 11. State, Equilibrium and Process The prefix “iso”- is often used to designate a process for which a particular property remains constant. Isobaric process: A process during which the pressure P remains constant. Pressure is Constant (ΔP = 0) Isobaric process: 11
  • 12. State, Equilibrium and Process Isochoric (or isometric) process: A process during which the specific volume V remains constant. Isochoric process: Isothermal process: A process during which the temperature T remains constant. Isothermal process: 12
  • 13. State, Equilibrium and Process Cyclic process - when a system in a given initial state goes through various processes and finally return to its initial state, the system has undergone a cyclic process or cycle. Reversible process – system can restored to it’s initial state from final state without the aid of any external agency. Irreversible process – once the final state reached, system can not reverse back to its initial state without the aid of external agency. Adiabatic process - a process that has no heat transfer into or out of the system. It can be considered to be perfectly insulated. 13
  • 14. Explanation of reversible process Reversible process 14 Key features of reversible process: • Driving and opposing force differ by infinitesimal amount. • Process occurs at very slowly & take infinite time to complete. • At every step, system attains equilibrium. • Most of the natural process are irreversible except phase changes ( melting/freezing of ice/water at 0°C & 1 atm pressure.
  • 15. Path function and state function 15
  • 16. Zeroth Law of Thermodynamics “ If two bodies are in thermal equilibrium with a third body, there are also in thermal equilibrium with each other.” 16
  • 18. WORK 18 Work done in reversible process for an ideal gas:
  • 19. First law of thermodynamics and internal energy The first law of thermodynamics states that the amount of heat given to a system is equal to the sum increase in the internal energy of the system and the external work done. Statement of the first law of thermodynamics  Conservation of energy.  Energy can neither be created nor destroyed but it can change forms.  Total amount of energy in a closed system remains constant. Description with formula Heat/work formula: ΔU=Q-W dU= ΔQ-PdV (W=PdV) 19
  • 20. Significance and limitation Significance:  The total amount of energy in the world is constant.  It is impossible to get more energy out of a system than is put into it.  You can’t get energy from nothing. Limitation: First law does not help to predict whether the certain process is possible or not. Reason: It does not specify that heat cannot flow from low temperature body to a high temperature body. 20
  • 21. Enthalpy(H) and Heat capacity (Cp & Cv) 21 Enthalpy: A thermodynamic quantity equivalent to the total heat content of a system is called enthalpy. Denoted by ‘H’. H=U+PV; where U is internal energy, P & V are pressure and temperature. Change in enthalpy; ΔH=ΔU+ΔPV ΔH = ΔU+PΔV+VΔP; at constant pressure, ΔH= ΔU+PΔV Classification of reactions based on ΔH Exothermic reactions (ΔH = (-) ve) (HCl+NaOH NaCl +H2O+heat) An exothermic reaction is a reaction that releases energy to the surroundings. 2. Endothermic reactions (ΔH = (+)ve) ;(N2(g)+O2(g) +heat 2NO (g)) An endothermic reaction is a reaction that absorbs energy from the surroundings.
  • 22. Enthalpy(H) and Heat capacity (Cp & Cv) 22 Heat Capacity: It is the amount of heat required to increase the temperature by 1° C. q = cΔT; the coefficient c is called heat capacity. Specific Heat Capacity: The amount of energy needed to increase the temperature of 1 gram of a material by 1 °C is known as its specific heat. q = m csΔT; q is heat, m is mass, ΔT is change in temperature, the coefficient cs is called specific heat capacity. CP and CV Specific heat capacity at constant pressure and constant volume. Relation between Cp and Cv: qP = nCP∆T = ∆H (1); qV = nCV∆T = ∆U (2) ∆H = ∆U + ∆(pV ) = ∆U + ∆(RT) = ∆U + R ∆T (for 1 mole ideal gas; PV=RT) ∆H = ∆U + R ∆T (3) Using the equn. 1&2 in 3, we get ; CP∆T = CV∆T + R ∆T CP –CV =R CP/CV =γ; γ is 1.6, 1.4 and 1.3 for mono, di and polyatomic gases.
  • 23. Standard Enthalpy(H⦵) and Thermochemistry 23 Various enthalpy changes: 1. Standard enthalpy change of reaction, ΔH° r (in general) 2. Standard enthalpy change of formation, ΔH°f 3. Standard enthalpy change of combustion, ΔH°c 4. Standard enthalpy change of neutralisation, ΔH°n 5. Standard enthalpy change of atomisation, ΔH°at 6. Standard enthalpy change of solution, ΔH°sol 7. Standard enthalpy change of hydration, ΔH°hyd Standard condition: Temparature298K and Pressure1 atm (~100 Kpa) Common interpretation: Enthalpy change of 1 mole substance  due to some physical process.