Thermodynamics Flashcards
(54 cards)
What is Thermodynamics based on?
Thermodynamic is based on initial and final states of a system undergoing the change. Laws of thermodynamics apply only when a system is in equilibrium or moves from one equilibrium state to another equilibrium state.
Define system and surroundings.
A system in thermodynamics refers to that part of universe in which observations are made and remaining universe constitutes the surroundings. Surroundings include everything other than the system.
Universe = System + Surroundings
What is boundary?
Wall that separates the system from surroundings.
Define types of system.
Open System: In an open system there is an exchange of energy and matter between the system and surroundings. The presence of reactants in an open beaker is an example of an open system. Here, the boundary is imaginary.
Closed System: In a closed system, there is no exchange of matter but exchange of energy is possible between the system and surrounding. The presence of reactants in a closed system made of conducting material (Cu/Fe) is an example of closed system.
Isolated System: In an isolated system there is no exchange of energy or matter between the system and the surroundings. The presence of reactants in a thermos flask or any other closed insulated vessel is an example of isolated system.
How is state of a system described?
The state of a system is explained by State functions or State variables. The state of a thermodynamic system is described by its measurable or microscopic (bulk) properties. They are called so because their values depend only on the state of the system and not on how it is reached.
What is Internal Energy?
The total energy of a system in thermodynamics is explained by internal energy; denoted by U,it may change when:
•heat passes into or out of the system
•work is done on or by the system
•matter enters or leaves the system
What is an Adiabatic system/process/wall?
Adiabatic system is an system where the transfer of energy between the system and surroundings is not possible or allowed.
Adiabatic process is a process in which there is no transfer of heat between the system and surroundings.
The wall separating the system and surroundings in such a case are known as adiabatic walls.
A: Work is a state function.
R: Work does depend on the path taken to do it.
Answer: (c) A is true but (R) is false.
As, work is a path function and not a state function.
A: Internal Energy is a state function.
R: Given amount of work done on the system no matter how it was done (irrespective of path taken), produces the same change of state.
Answer: (a) A is True and (R) is true and (R) is the correct reason.
Give expression for Work Done in adiabatic system and Internal Energy .
∆U = U2 - U1 = Wad
The positive sin expresses that W is positive when work is done on the system and the internal energy of the system increases. If the work is done by the system W will be negative because the internal energy of the system decreases.
Explain Heat in Thermodynamics.
Exchange of energy, which is a result of temperature difference is called heat (q).
Heat absorbed by the system (water), q can be measured in terms of temperature difference:
T2 - T1
Also, ∆ U = q when no work is done at constant volume.
Is temperature (T) a state function or a path function, what about volume (V)?
Both are state functions.
Explain the First Law of Thermodynamics (FLOT).
It states that:
The energy of an isolated system is constant.
Also commonly stated as law of conservation of energy; i.e. energy can neither be created nor be destroyed.
It’s independent of the way the change is varied out (path).
Expression:
∆ U = q + w
∆ U = 0 when, no transfer of energy or work done (isolated system).
We cannot determine the absolute value of a system’s internal energy, only the change in internal energy that occurs during a process because there is no absolute reference point to measure it against; we can only measure the difference in internal energy between two states.
Explain W.D. on an ideal gas inside a cylinder getting compressed.
Cylinder which contains one mole of an ideal gas fitted with a frictionless piston. The total volume of the gases Vi and pressure of the gas inside is P if external pressure is Pex which is greater P. Piston is moved inward till the pressure inside becomes equal to Pex.
Vol. Change: l(dis. moved by piston) × A = ∆ V = (Vf - Vi)
Force = Pex • A (P = F/A)
Work Done = f × dis = Pex • A • l
Work Done = -Pex(Vf - Vi) = -Pex(∆V)
The negative sign of this expression is required to obtain a conventional sign for work done which will be positive. It indicates that in case of compression work is done on the system.
Explain importance of negative sign in the formula for work done in relation to gas inside a cylinder.
Expression: Work Done = -Pex(Vf - Vi) = -Pex(∆V)
The negative sign of this expression is required to obtain a conventional sign for work done which will be positive. It indicates that in case of compression work is done on the system.
Explain reversible process wrt Thermodynamics.
A process or change said to be reversible for changes brought out in such a way, that the process could at any moment, be reversed by an infinitesimal change. Reversible process proceeds infinitively slowly by series of equilibrium states such that the system and the surroundings are always in near equilibrium with each other.
When can we form a relation between work and internal pressure? Explain the relation.
We can form a relation between work and internal pressure of the system under reversible conditions.
Wrev = -nRTln(Vf/Vo)
Wrev = -2.303 nRT log(Vf/Vi)
Explain Free expansion.
Expansion of a gas in vacuum is called free expansion. No work is done during the expansion of an ideal gas (since, Pex = 0) whether the process is reversible or irreversible.
At constant volume: ∆ U = q
Here, q = qv = heat supplied at constant volume.
Explain isothermal and free expansion of an ideal gas.
For isothermal expansion (T constant) of an ideal gas into vacuum, w = 0 since Pex = 0. Also, experimentally derived that q = 0.
Expression for isothermal reversible change:
q = -w = -Pex(Vf/Vi)
Expression for isothermal irreversible change:
q = -w = nRTln (Vf/Vi) = 2.303 nRT log(Vf/Vi)
For adiabatic change (q = 0):
∆U = Wad
Explain Enthalpy wrt Thermodynamics.
When heat is absorbed by the system at constant pressure we are measuring changes in Enthalpy (∆H).
Enthalpy (H) expression:
H = U +pV
∆H = ∆U + p∆V (p constant)
q = ∆H = H2 - H1
Here, q = q(p) = heat absorbed by the system.
Also, we know **heat is a path function but clearly, heat absorbed by system [q(p)] is a state function. **
Also, ∆H is a state function.
∆H is negative for exothermic reactions which evolve heat during the reaction and is positive for endothermic reactions which absorb heat for the surroundings.
At constant volume:-
For solids and liquid: ∆H = ∆U = qv
For gases: ** ∆H = ∆U + ∆n(g)RT
Here, n(g) means no of moles of gaseous products - of gaseous reactants.
Differentiate between extensive and intensive properties.
Extensive property is a property whose value depends on the quantity or size of matter present in the system, ex; mass, volume, internal energy, enthalpy, heat capacity, etc.
Properties which do not depend on the quantity or size of the matter present or known as intensive properties; ex: temperature, density, pressure, etc.
Explain Heat Capacity.
We know increasing temperature is proportional to heat transferred.
q ∝ k × T
The constant or coefficient ‘k’ here is Heat Capacity (C).
q = C ∆T
A large heat capacity means a lot of energy is needed to raise its temperature.
Explain Molar Heat Capacity.
Molar heat capacity of a substance is the heat capacity for one mole of the substance and in the quantity of heat needed to raise the temperature of 1mol by 1degree Celsius or 1Kelvin.
Cm = (C/n)
Where, Cm = Molar Heat Capacity.
C can be derived from; q = C ∆T
Explain Specific Heat Capacity.
Specific heat capacity is the quantity of heat required to raise the temperature of 1 unit mass of a substance by 1degree Celsius or 1Kelvin.
q = c × m × ∆T = C ∆T
Here, small c (c) is specific heat capacity.