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02 part4 work heat transfer first law prob
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Work Transfer
S.Gunabalan Associate Professor Mechanical Engineering Department Bharathiyar College of Engineering & Technology Karaikal - 609 609. e-Mail : [email protected]
Part - 2
Short Note • 푝푉 = 퐶
– 푛 log =log • P1,P2,t1,m Given
– Find V1 • 푝1푉1 = 푚푅푇1
푅 = 푅/M V2 – Final volume The conditions are
– Cylinder size : 280 diameter (D) – As the piston moves a distance of 305 mm (h)
푉2 = 휋푟 ℎ
Process in which pV n = C 푾ퟏퟐ =
푷ퟏ푽ퟏ − 푷ퟐ푽ퟐ풏 − ퟏ
Mass of steam 0.02 Kg (m) P1 = pressure of 0.6MPa (p1) temperature of 200 oC (T1) p2 = 0.12MPa
푝1푉1 = 푚푅푇1 0.6푀푃푎푥푉1 = 0.02퐾푔푥푅푠푡푒푎푚푥 200 + 273 퐾
푹 = 푴푹 푹 = 푹/M 푹− 푼풏풊풗풆풓풔풂풍푮풂풔풄풐풏풔풕풂풏풕푲푱 푲.풎풐풍푲⁄
푹 = ퟖ.ퟑퟏퟒퟒퟏ푲푱 푲.풎풐풍푲⁄
푴 − 푴풐풍풆풄풖풍풂풓풘풆풊품풉풕푲품 푲.풎풐풍
퐑 − 퐜퐡퐚퐫퐚퐜퐭퐞퐫퐢퐬퐭퐢퐜퐠퐚퐬퐜퐨퐧퐬퐭퐚퐧퐭 푲푱 풌품푲
Gas Molar Weight ( M)Kg/Kmol
Air 28.97
Nitrogen 28.01
Oxygen 32
Hydrogen
2.016
Helium 4.004
Carbon dioxide
44.01
Steam 18.02
pdV-Work - Quasi-Static Processes
Process in which pV n = C 푾ퟏퟐ =
푷ퟏ푽ퟏ − 푷ퟐ푽ퟐ풏 − ퟏ
Process in which pV = Constant
푾ퟏퟐ = P1V1 퐥퐧 푽ퟐ푽ퟏ
OR 푾ퟏퟐ = P1V1 풍풏 푷ퟏ
푷ퟐ
Constant Volume process (isochoric process) dV = 0 푾ퟏퟐ = 0 Constant pressure process (isobaric) 푾ퟏퟐ = p(v2-v1)
Ex-4 A fluid is confined in a cylinder by a spring loaded frictionless piston so that the pressure in the fluid is a linear function of volume
푝 = 푎 + 푏푉 The internal energy of the fluid is given by the following equation
푢 = 34푎 + 3.15푝푉 Where 푢푖푛퐾퐽, 푝푖푛푘푃푎푎푛푑푉푖푛푚3. Find the fluid change from an initial state of 170kPa 0.03m3 to a final state of 400kPa, 0.06m3 with no work other than, that done on the piston. Find the direction and magnitude of the work and heat transfer.(Apr/May 2011)
Given Data 푝 = 푎 + 푏푉
푢 = 34푎 + 3.15푝푉 Where 푢푖푛퐾퐽,푝푖푛푘푃푎푎푛푑푉푖푛푚3. P1 = 170kPa V1 = 0.03m3 P2 = 400kPa, V2 = 0.06m3
work = ? heat transfer = ?
a, b – two constant need to be addressed 푝 = 푎 + 푏푉
Where 푢푖푛퐾퐽,푝푖푛푘푃푎푎푛푑푉푖푛푚3. P1 = 170kPa V1 = 0.03m3
푝 = 푎 + 푏푉 170 = 푎 + 0.03푏 −− −(1)
P2 = 400kPa, V2 = 0.06m3
400 = 푎 + 0.06푏 −− −(1) Find a,b
Work Done
푊12 = 푝푑푣
푝 = 푎 + 푏푉
푊12 = 푎 + 푏푉 푑푣
푊12 = 푎 푉2 − 푉1 + 푏(푉2
2− 푉2
1
2)
Heat transfer Q 푄 = ∆푢 + 푤12
푢 = 34푎 + 3.15푝푉
∆푢 = 푢2 - 푢1
∆푢 = (34푎 + 3.15푝푉)2 – (34푎 + 3.15푝푉)1 ∆푢 = 3.15[(푝푉)2 – (푝푉)1] Substitute and find Q
푄 = ∆푢 + 푤12
Reference • Nag, P. K. 2002. Basic and applied thermodynamics. Tata McGraw-Hill, New
Delhi.