Development of Balance Equations for Mass, Energy, and Entropy: Application to Closed-Steady SystemsĢ.3 Cycles-a Special Case of Closed-Steady Systemsģ.

Microscopic Thermodynamicsġ.5.1 Property Evaluation by State Daemonsġ.5.2 Properties Related to System Size (V, A, m, n, m #, V#, n # )ġ.5.7 Stored Energy (E, KE, PE, U, e, ke, pe, u, E#)ġ.5.8 Flow Energy and Enthalpy (j, J#, h, H#)Ģ.

Description of a System: States And Propertiesġ.3 Macroscopic vs. Introduction Thermodynamic System and its Interactions with the SurroundingsĠ.4 Interactions Between The System and its Surroundingsġ. Check with the seller prior to purchase.Ġ. If you rent or purchase a used book with an access code, the access code may have been redeemed previously and you may have to purchase a new access code.Īccess codes that are purchased from sellers other than Pearson carry a higher risk of being either the wrong ISBN or a previously redeemed code. In addition, you may need a CourseID, provided by your instructor, to register for and use Pearson's MyLab & Mastering products.Īccess codes for Pearson's MyLab & Mastering products may not be included when purchasing or renting from companies other than Pearson check with the seller before completing your purchase. Several versions of Pearson's MyLab & Mastering products exist for each title, including customized versions for individual schools, and registrations are not transferable. As in part (b.) but with the two steps performed in opposite order.ALERT: Before you purchase, check with your instructor or review your course syllabus to ensure that you select the correct ISBN. The volume is increased and heat is supplied at just the right rate to make the pressure decrease linearly with volume.ĭ. (Heat must be extracted from the system during this stage of the process.)Ĭ. (Heat must be added to the system during this expansion in order to keep the pressure constant.) Then at constant volume, the the pressure is reduced from p i to p f. At constant pressure, the gas expands from V i to V f. Find the total work done on the system and heat absorbed by the system in each of the following quasistatic processes, all of which connect the same two thermodynamic states.Ī.

Of course, this is not the only process leading from this particular initial state to that particular final state.

Interactive thermodynamics 3.2