Presentation on theme: "Laws of Thermodynamics"— Presentation transcript:
1 Laws of Thermodynamics Lecture 1Laws of ThermodynamicsThermodynamic state - equilibriumThermodynamic processesLaws of thermodynamicsAbsolute TemperatureProblems 2.5, 2.6, 2.8
2 Thermodynamic state - equilibrium Thermodynamic intensive coordinates are uniform across the whole system (T, P, ) or across each macroscopic phase (e.g., water and ice density density at the melting point.All thermodynamic coordinates are time independentMechanical equilibrium, thermal equilibrium and chemical equilibrium
3 Macroscopic vs. microscopic state Thermodynamic coordinates (T, P, ) define macroscopic state of equilibrium.Microscopic state is defined by atomic positions, and momenta - many microscopic states are consistent with a macroscopic stateStatistical mechanics connects microscopic description and detail with macroscopic state via ensemble average
4 Thermodynamic process change of the thermodynamic state Infinitesimal process infinitesimal change of coordinates, e.g., dT, dV, dPQuasi static process always near equilibriumAdiabatic process no heatReversible process can be restored to the initial state without charging surroundings
5 0th law of thermodynamics Two or more systems in equilibrium do not exhibit heat flow among each other, they are at the same temperatureLater we will see that criterion of equilibrium for isolated system, i.e., const E, V, T is the maximum entropy statedS(E, V, N) = 0dS = dS1+dS2 = 0Allowing only energy exchange between two isolated systemsE1, V1, N1E2, V2, N2From conservation of energy
6 1st law of thermodynamics - conservation of energy dE = dQ-dWd indicates inexact differential - depends on the integration pathIn a cycle, E = 0net Q in = net W outWork and heat are not state functionsEnergy is a state functiondW = Fdx can be PdV, -dl, -it
7 2nd law of thermodynamics - entropy For a reversible processdQ= TdSWhere S is entropy which a state function, and T is an absolute temperatureThe entropy can by calculated by integrating heat over a reversible path
8 Absolute temperature Consider the Carnot cycle Since entropy is the state functionQ1TST1T2Q2Using reference T3 = KQ > 0
9 Problem 2.5When a system is taken from a to b state along abc 80 joules of heat flows into the system and the system does 30 joules of work.How much heat flows into the system along path adb, if the work done by the systems is 10 joules.When the system is returned from b to a along the curved path the work done on the system is 20 joules. Does the system absorb or liberate the heat? How much?If Ea = 0 and Ed = 40 joules, find the heat absorbed in process ad and db.cbPVAnswers:Qadb = 60 joules.Qba = - 70 joules joules (liberate heat) of the heatQad= 50 J, Qdb= 10 Jad
10 Problem 2.6A vessel of volume VB contains n moles of gas at high pressure. Connected to the vessel is a capillary tube trough which the gas may slowly leak out into the atmosphere, where P=P0. Surrounding the vessel and capillary is a water bath, in which is immersed an electric resistor. The gas is allowed to leak slowly trough the capillary into the atmosphere while, at the same time, electrical energy is dissipated in the resistor at such a rate that the temperature of the gas, the vessel, the capillary and the water is kept equal to that of the surrounding air. Show that, after as much gas is leaked as is possible during time , the change of internal energy iswhere, v0 = molar volume of gas at P=P0, = potential on the resistor, and i is the current.
11 Problem 2.8The tension force in a wire is increased quasi statically and isothermally from 1 to 2. If the length, cross-sectional area and isothermal Young’s modulus (Y) remain practically constant, show that the work done by the wire is:
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