Physical Chemistry 2 Flashcards
What is thermodynamics?
The study of energy transformations
What is energy and work?
Work - a form of energy which can transfer in and out of a system, stored in the organized motion of molecules.
It is done when an object is moved against as opposing force.
Energy - capacity to do work. Energy of a system can be changed by work and heat.
How is work done calculated / defined?
W = Fx
By definition;
dW = -Fdz
and pressure, P = F/A
So by substitution,
dW = -PAdz
and Adz has units of volume (x³)
Therefore dW = -PdV
Which can then be integrated
What’s a diathermic and adiabatic system?
Diathermic - energy can transfer in and out as heat
Adiabatic - no heat can be transferred in and out
What’s internal energy?
Total energy of a system, as a function of state, and is an extensive property (dependent on the amount of matter).
For an adiabatic process, what is internal energy equal to?
Overall energy balance:
ΔU = Q + W
However ΔQ is 0 as there is no transfer of heat so:
ΔU = W
For an isobaric process, what is internal energy equal to?
Overall energy balance:
ΔU = Q + W
Both still exist for this process (although ΔP is 0)
What is an isochoric process?
One with a constant volume.
ΔV = 0
For an isochoric process, what’s internal energy equal to?
Overall energy balance:
ΔU = Q + W
However, ΔV = 0 (and W=PΔV)
Therefore:
ΔU = Q
For an isothermal process, what is internal energy equal to?
Temperature is fixed (ΔT = 0) and it’s energy stays constant so ΔU = 0
Therefore:
Q = -W
For an cyclic process, what is internal energy equal to?
Certain processes have the same initial and final states, represented by a closed path and ΔU = 0.
Therefore:
Q = -W
What’s a reversible and irreversible process?
Reversible - the system is never more than infinitesimally far from equilibrium and an infinitesimal change in external conditions can reverse the process
Irreversible - cannot be reversed by an infinitesimal change in external conditions
How can work by an ideal gas be calculated?
Using pV = nRT and W = pΔV
How is heat capacity at constant volume defined/calculated?
Cᵥ = (dU/dT)ᵥ = Q v
->
dU = CᵥdT
For a certain range of T where Cv is constant
No work is done
What’s molar heat capacity and specific heat capacity (how is it found)?
Molar: C vm = Cv / n
Specific heat is in terms of mass