"Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor

ABSTRACT Isothermal reversible thermodynamic processes were studied, where there will not occur flow of heat (q) in the system in accord with the second law of thermodynamic. It appear that the energy flow in the system cannot be explained adequately by considering the flow of P,V � work, usually...

وصف كامل

محفوظ في:
التفاصيل البيبلوغرافية
المؤلف الرئيسي: Perpustakaan UGM, i-lib
التنسيق: مقال NonPeerReviewed
منشور في: [Yogyakarta] : Universitas Gadjah Mada 2003
الموضوعات:
الوصول للمادة أونلاين:https://repository.ugm.ac.id/18325/
http://i-lib.ugm.ac.id/jurnal/download.php?dataId=1107
الوسوم: إضافة وسم
لا توجد وسوم, كن أول من يضع وسما على هذه التسجيلة!
المؤسسة: Universitas Gadjah Mada
id id-ugm-repo.18325
record_format dspace
spelling id-ugm-repo.183252014-06-18T00:31:03Z https://repository.ugm.ac.id/18325/ "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor Perpustakaan UGM, i-lib Jurnal i-lib UGM ABSTRACT Isothermal reversible thermodynamic processes were studied, where there will not occur flow of heat (q) in the system in accord with the second law of thermodynamic. It appear that the energy flow in the system cannot be explained adequately by considering the flow of P,V � work, usually indicated by w, in accordance with the first law, that is, AU = q + w with q = 0. Therefore, it is necessary to have another kind of work energy (potential) which is not electrical to explain such as the experiment of Boyle that results in the formula PV = C for a close ideal gas system undergoing an isothermal and reversible process. In this paper, a new work potential which is called "terpi" is introduced, and is abbreviated as 2- (tau) and defined as: dr - T dS�v = - dq�,,. Therefore, dr is also not an exact differential as dw and dq. For any isothermal reversible process, it can be written: 2- = -TAS,ev, and for redox reaction, such as an electrochemical cell, it is noteworthy to distinguish between Z system (2-eyed and z reaction (2-,) which combine together to become an electrical work flow, (wet) done by the system on the surrounding, so that: AG,= Tsyst + Tr =V FE Furthermore, the studies of phase transitions, which occur isothermally, were also considered, e.g. the evaporation of a liquid into vapour at a certain T. The heat given to this process cannot freely flow isothermally, but first it must be changed into terpy and then added to the enthalpy .of the vapour following the equation: 2-vap = -ThSvap -AHvap. Keywords: thermodynamics, heat, work, isothermal, reversible [Yogyakarta] : Universitas Gadjah Mada 2003 Article NonPeerReviewed Perpustakaan UGM, i-lib (2003) "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor. Jurnal i-lib UGM. http://i-lib.ugm.ac.id/jurnal/download.php?dataId=1107
institution Universitas Gadjah Mada
building UGM Library
country Indonesia
collection Repository Civitas UGM
topic Jurnal i-lib UGM
spellingShingle Jurnal i-lib UGM
Perpustakaan UGM, i-lib
"Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
description ABSTRACT Isothermal reversible thermodynamic processes were studied, where there will not occur flow of heat (q) in the system in accord with the second law of thermodynamic. It appear that the energy flow in the system cannot be explained adequately by considering the flow of P,V � work, usually indicated by w, in accordance with the first law, that is, AU = q + w with q = 0. Therefore, it is necessary to have another kind of work energy (potential) which is not electrical to explain such as the experiment of Boyle that results in the formula PV = C for a close ideal gas system undergoing an isothermal and reversible process. In this paper, a new work potential which is called "terpi" is introduced, and is abbreviated as 2- (tau) and defined as: dr - T dS�v = - dq�,,. Therefore, dr is also not an exact differential as dw and dq. For any isothermal reversible process, it can be written: 2- = -TAS,ev, and for redox reaction, such as an electrochemical cell, it is noteworthy to distinguish between Z system (2-eyed and z reaction (2-,) which combine together to become an electrical work flow, (wet) done by the system on the surrounding, so that: AG,= Tsyst + Tr =V FE Furthermore, the studies of phase transitions, which occur isothermally, were also considered, e.g. the evaporation of a liquid into vapour at a certain T. The heat given to this process cannot freely flow isothermally, but first it must be changed into terpy and then added to the enthalpy .of the vapour following the equation: 2-vap = -ThSvap -AHvap. Keywords: thermodynamics, heat, work, isothermal, reversible
format Article
NonPeerReviewed
author Perpustakaan UGM, i-lib
author_facet Perpustakaan UGM, i-lib
author_sort Perpustakaan UGM, i-lib
title "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
title_short "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
title_full "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
title_fullStr "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
title_full_unstemmed "Terpi" As A Quantity Of Thermodynamic Potential Energy Supplementary To The Concept Of Work And Heat = Besaran "Terpi" Sebagai Energi Potensial Termodinamika yang Melengkapi Pengertian Kerja dan Kalor
title_sort "terpi" as a quantity of thermodynamic potential energy supplementary to the concept of work and heat = besaran "terpi" sebagai energi potensial termodinamika yang melengkapi pengertian kerja dan kalor
publisher [Yogyakarta] : Universitas Gadjah Mada
publishDate 2003
url https://repository.ugm.ac.id/18325/
http://i-lib.ugm.ac.id/jurnal/download.php?dataId=1107
_version_ 1681217248484655104