thermodynamics_process - THERMODYNAMIC PROCESSES When any...

Info iconThis preview shows pages 1–2. Sign up to view the full content.

View Full Document Right Arrow Icon
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
Background image of page 2
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: THERMODYNAMIC PROCESSES When any one of the three parameters P, V or T: varies we claim that a thermodynamic process has occurred. We need to take a deeper look at the process. We begin by recognizing that if you (P ' Wish to represent the state of a system by a point (such as A) on a P-V diagram, A the system must be in equilibrium 0 otherwise temperature is not the same every where and therefore P and V are not unique.This has the immediate implication that if you represent a thermodynamic process by a continuous , line the system must in equilibrium at _ WWW, ' ’ % every point along the way from initial V state I to final state F. ' l3 Eam‘t‘u‘b‘ Rim/«.4 #7“ . . EMMY Pry/WT @ETWEEA/ — 1551;0ch How can We do that? The process must be carried out infinitely slowly. For example, if I~> F is an adiabatic expansion you can imagine starting at I, reducing the pressure by removing one electron [mass = 9 x 10’3 1 kg] fiom the piston at a time and repeating this ever so small step to eventually reach F. Since the system is in E m at every point, one can stop any where and go forward or back because each step is infinitesimal. Such a process is therefore REVERSIBLE. Hence the arrow is pointing both ways in diagram above. However, such a process will take forever, so it is only an IDEAL. In a real process which must be carried out over small time intervals we ensure equilibrium only in the initial and final states. Hence, it is represented by two points on PV diagram. ‘H . There is no information about any of the intermediate points. This is a or LABORATORY process, but now we have no way of getting back to I so this process is IRREVERSIBLE. > ...
View Full Document

This note was uploaded on 12/28/2011 for the course PHYSICS 121 taught by Professor Shawhan during the Spring '10 term at Maryland.

Page1 / 2

thermodynamics_process - THERMODYNAMIC PROCESSES When any...

This preview shows document pages 1 - 2. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online