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1st Law of Thermodynamics

Energy can be neither created nor destroyed (conservation of energy)

Thus power generation processes and energy sources actually involve conversion of energy from one form to another, rather than creation of energy from nothing

ΔQ = ΔU + ΔW

ΔU: Change in internal energy of the system

ΔQ: Heat transferred into/out of the system

ΔW: Work done by/on the system

 

Thermodynamics

Cylinder has area, A. A fluid is admitted at constant pressure, p

p = F/A & Wd = fd … rearrange:

F = pA → Wd = pAd (Ad = volume, V)

→ Wd = pV or ΔWd = pΔV

 

pV = nRT (Ideal Gas Law)

Boyle’s Law: pV = constant

  • Temperature remains constant (isothermal)
  • pV = constant and p1V1 = p2V2
  • ΔU = 0 because the internal energy is dependent on temperature, which does not change
  • ΔQ = ΔW. If the gas expands to do work ΔW, & amount of heat ΔQ must be supplied
  • compression or expansion produces the same graph

Adiabatic: no heat flow (ΔQ=0) into or out of a system

For a change in pressure or volume in a system, the temperature loss can be calculated:

p1V1/T1 = p2V2/T2

At high p, low V: adiabatic = value expected for isothermal at high T

At low p, high V: adiabatic cuts isothermal at low T

Adiabatic Compression

Equation for adiabatic line:

pVγ = k

γ = Cp/Cv

k= constant

 

Isovolumetric: p1T1 = p2T2

Isovolumetirc

Isobaric: V1T1 = V2T2

Isobaric