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Derive the seven general property equation of the following thermodynamics processes: a. ISOTHERMAL PROCESS - Any Process relation - Work Non-flow - Internal Energy - Heat Transferred - Enthalphy - Entropy - Work Steady flow refer with the picture. Show the detailed explanation please

Derive the seven general property equation of the following thermodynamics processes: a. ISOTHERMAL PROCESS - Any Process relation - Work Non-flow - Internal Energy - Heat Transferred - Enthalphy - Entropy - Work Steady flow refer with the picture. Show the detailed explanation please

Elements Of Electromagnetics
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
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Derive the seven general property equation of the following thermodynamics processes: a. ISOTHERMAL PROCESS - Any Process relation - Work Non-flow - Internal Energy - Heat Transferred - Enthalphy - Entropy - Work Steady flow refer with the picture. Show the detailed explanation please
3. Isothermal Process AU = 0 Isothermal process is the process applied to ideal gas by which - Heat Transferred: the temperature is held constant and from this process, the 7- Following the relation of heat transfer, we have: general equations can be related to the process as follow: Q=0+ W. * Any Process relation: Q = w, - PVin A = MRTIN = mRTin A | = PV = C * Enthalpy: P,V = P,V2 Since there is a constant temperature, we have an enthalpy of: V Pz V2 P AH = 0 * Entropy: v Work Non-flow: Following the guiding equation as represented by the to obtain For process relation, by holding the temperature constant under AS, this process, we can have T=Cand that so employing again the S- integral, wherein we have: W, = [Pav Pdl Q = mRTin #) = mRTIn ) from process definition: Evaluating to obtain the change in entropy, PV" = C where n =1 (isothermal) PV = C AS = mRin #) = | mRine P = - Work Steady flow: For work steady flow, we follow the integral below: substituting to the integral and evaluating: W, = - W. - [av = c [ w. = PVin 4)- AP: Also, from process definition: = MRTI PV" = C wheren = 1 (isothermal) PV = C and where PV can be either obtain from state point 1 or 2. v Internal Energy: V = Since there is a constant temperature, we have an internal energy substituting to the integral and evaluating: of: dP w, = PVin A = MRTIN = MRTIN From the derived relation, we conclude that in isothermal process non-flow work is equal to work steady flow. W, = W.
Transcribed Image Text:3. Isothermal Process AU = 0 Isothermal process is the process applied to ideal gas by which - Heat Transferred: the temperature is held constant and from this process, the 7- Following the relation of heat transfer, we have: general equations can be related to the process as follow: Q=0+ W. * Any Process relation: Q = w, - PVin A = MRTIN = mRTin A | = PV = C * Enthalpy: P,V = P,V2 Since there is a constant temperature, we have an enthalpy of: V Pz V2 P AH = 0 * Entropy: v Work Non-flow: Following the guiding equation as represented by the to obtain For process relation, by holding the temperature constant under AS, this process, we can have T=Cand that so employing again the S- integral, wherein we have: W, = [Pav Pdl Q = mRTin #) = mRTIn ) from process definition: Evaluating to obtain the change in entropy, PV" = C where n =1 (isothermal) PV = C AS = mRin #) = | mRine P = - Work Steady flow: For work steady flow, we follow the integral below: substituting to the integral and evaluating: W, = - W. - [av = c [ w. = PVin 4)- AP: Also, from process definition: = MRTI PV" = C wheren = 1 (isothermal) PV = C and where PV can be either obtain from state point 1 or 2. v Internal Energy: V = Since there is a constant temperature, we have an internal energy substituting to the integral and evaluating: of: dP w, = PVin A = MRTIN = MRTIN From the derived relation, we conclude that in isothermal process non-flow work is equal to work steady flow. W, = W.
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