d d / d d d ^ ' d d d /D' d d d h ' d d d d d d ^ d d ^ e d d e d d e d d d d d d d W d d, de d d & de d d W d d d d d W d d & d e d /D e de e d de e
|
|
- Dale Hoover
- 5 years ago
- Views:
Transcription
1 hzkwekdd/^^/ke /ZdKZd 'EZ> >/D/KE / D ' d h d^ ' & d
2 d d / d d d ^ ' d d d /D' d d d h ' d d d d d d ^ d d ^ e d d e d d e d d d d d d d W d d, de d d & de d d W d d d d d W d d & d e d /D e de e d de e d de e d ^ d: de e d e de e d d / de e d d,w de e d d de d
3 d / d d ^ ' d D ^ h W /// hd^ K: d d h d^ /D E / D E/D d d E> & /^/ / d t ' t'/// D ^ / d D ^ / ',' D ^ d d /D' ^ /D d /D d /// d /D /D d / ' d ' d ' d / d
4 ' d E/D E / D d ' d ' e ' e ' e ' e /D d W /// hd^ ' / / h d^ ' Z hd^ /D d d h ' d W /// hd^ D ^ e /D E / D E/D d ee d d E D ^ d ee d
5 &Y d d ^ & d W, & W d
6 d d ^ d d d d d d d e d e
7 d d D s W, & ^ / /D ed d d: de d d: / /D, d - d - d - d - d e - d -, d^ d^ KZ d^ d^, d^ K D ' e & d - d - d - d - d KZ KZ Z e
8 d d D s W d ee W d - d - d K d / ee / /D K d K K d K d K K d K D/Eh^ ' e o d o d o d o o d o d Z E e
9 d ^ d d le ^ /D d d d d ' d / ^ ' d / d d ^ d & & / ' d e > > / // /D > & >& & ' d E D >& ' d > e
10 ^ d d / t / CO 2 Production process Benchmarked Product 1 Fuel Heat CO 2 Production process Benchmarked Product 2 d d ^ d K d d d E K E d
11 - d^ - - d d^ - - D d & ' d d E d E d E E,W / d^ d DW hd^ d d d^ ',' d t
12 ' d ^ d d d & d^ d d ^ d d K d D D / D D > d d d E d
13 d d K K W d d ^ W E e E & t ^ ' d ^ d d d ^ d d K d K d / ee EdK Kd h d^ d d d E d
14 EdK ' t W d d K d d d K d d d d D/Eh^ ^ ' e t ' t ' d d d d /D Z h W W W
15 & d / K d K d, e ^ d e / d W W & d^
16 d d & e d d W & d d d CO 2 Natural gas Fuel oil Heat Production process Benchmarked Product & d W ^ d d,> W /D ' e ^ d d & = DW,> t h & D W h,>, de
17 ^ ' e ^ ^ ' / / & d & d / / d /D ' e / + E, / & W = DW,> W + E, / + t & W h DW W h,> W, de
18 d de de d d^ d^ d^ E, / d^ d^ / K d E, / = E, / ed d t E, / d^ d^ d: d de de / / K d = d ded t Dt d de de / d^ d d^ d d^ ^ ' e de
19 d d, & d d d CO 2 Natural gas (TJ) Fuel oil (TJ) Heat (TJ) Production process & d, ^ d Non benchmarked Product d,> d: - d^ - E d^ ^ ' e / d d / ^ ' d ^ d & = D,> de
20 & W h D, ed d K d d: K / d^ d^ / d^ ^ ' e d d & & d d d CO 2 Natural gas (TJ) Production Non Fuel oil (TJ) benchmarked process Product Heat (TJ) & d & ^ d d,> d: d & /
21 , & ' e ^ d i & = D,> & W h D & de d K d d:,>, d: d d W & d d d Non-CO 2 CO 2 CO (incomplete combustion) & d Reducing agent (TJ) Heat (TJ) Production process W Non benchmarked Product ^ d d,> K d K d / ee K d d d
22 d d D/Eh^ d & ' e ^ d & = WZ&,> W & WZ& Z d ee,>, K d & K d / K K d K d / edl K d / ' e
23 d d d d = & & & d & i E/D d d W d ( ) & & & t = & W & & > & d d & & = & & ^& t & & ^&
24 & & = & d ed & t & & & W
25 d e d /D d - - d e d /D & e d d /D ^h& d ^ d d d d d D d t d : de / / /D dl E e d d d : de d d d D d
26 D d d : de d d / ' d / d de d / d d d & ^h& d de
27 e d ^ e d ^ e d ^ e d e d e d / de de e d /D d d e d e d d d e d d de de,>l de KZ,>l de / e e /D d ^ e e d d ^,> d de
28 d ^ de d d de d d, de de de e e d d d d e e d /,> e e,> l de e e d d ld,> l de d d e e ld d,> e W e e W /D d d d d de d d, de de de E e d d e h d e d d d d d d de
29 d ^ de /,> e e,> l de e d d e le,> l de d e d d ld,> l de d d d d ld > d e e W /D : d: d de de de de e e e e e e e d d e e e e e e e e e d d,> e W d, e d ^ d: d,> d d: d: e d de
30 d d /D & ed ed l d ed ed d / ed ed d & d e e &, >,> d d d d d / d / de d : de d,> d,> d,> > d,>l > > de > de > de de >deld,>l > > de > de K de,> de de de,>l > de > de > de
31 d / d / d : de d d de d,> de K,> e e /D,>l Zh& t d Zh& / d : de d,> d d d d : / : d d / ^ / Zh& de d d Zh& l / & Zh& d
32 / D d d & & / Zh& d Zh& E Zh& dl d
33 ^ d d ^, de de D e d de D e d de de de e e de D e d de de D e d de de de e e e d e e d : : / K ^ d ^ d d d d
34 ^ d, d: : e e : : d d d W d d e d l W d e d d d d dl d l d dl d td l d td
35 ^ d d / d d d d d / d & d W E d d dl
36 & d de & l e d E, d, d: & / & de e e / l ^ d d - l KZ - d dl W d l d de
37 / d / d ed t d / d e d d ^ / d & e d & e d Z d ^ // / > e t ^ / / e / de
38 ^ /// > AL = AL AL aed, design Total average / d ed ed l > md d ed l > md d d d e d Aed design capacity (C aed,design ) Initial capacity (C initial) Initial capacity (C initial) & e Remaining design capacity (C remaining,design ) de
39 E l d W d d d dl d de de d ^ d K d dl / e e d d / d d ^ d d & e l de
40 d Aed capacity (C aed ) New capacity (C new ) Initial capacity (C initial) & e / d & e l / Z E & e / / d d d / d d d d l ^ d K d d d,> e e
41 ,> l,> l,> t,> d de de,> d E,> /,>,> d,>,>,> / de de,> l & & t ^ / / >,h& ALinitial = Cinitial HCUFinitial,> / d
42 ,> d,h&,> l,h& d,h&,h& l & d,h& d,h& / e d,> /,> l d,h& d : de / : de / l d / lde d e l le
43 z de de de d W de ^ z de de de / d e e d de de d W de l,h& ^,> &,>,> l de de de l ^,h&,h& l l ^,>,> l,h& le ld ^,>,> l,> l,> lldl d : de / : de / l d / le d e Z l l e
44 z de de de d W e d ^ z de de de E e e Z e e / d W e d e ^,> &,>,> l de de l ^,h&,h& l l ^,>,> l d,h& l d e l d ^,>,> l,> l,> l dld d d / d : de d de & e / ld d / d lded d e & d l d led
45 / d ld d e ^ d l d d l z de de de d W ed ded d d C a2 C a1 C new2 C new1 C initial & e d ^ z de de de / d d d d d d ed ed ed d d d d ded d d d W ed ded d d l,h& ed ed ed ed ^,> &,>,> l de led ^,h&,h& l led d E,h& ^,> d,> d,> d l d,h& led ed dlee,> d l d,h& l ed dlde d
46 ^,>,> l,> l,> d l,> d ledlee dlde dle d de
47 e d e d d / CO 2 Natural gas (TJ) Product A - no benchmark - exposed to carbon leakage Fuel oil (TJ) Heat (TJ) Process Product B - no benchmark - exposed to carbon leakage Product C - no benchmark - NOT exposed to carbon leakage &, ^ / > d, > d, > d & > d & > d,> d,> d,> d,> d de
48 & ' d e d d,w /,W & d d d,w d^ d^ d,w d^ K,W E,W ^ ' e d^ /,W d^ d d^ d^ CO 2 Electricity Fuel CHP Heat Non-ETS consumer & ^,W ETS consumer de
49 e d d & d Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS ext heat Consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Fuel Waste gases Heat Electricity - d - - d - d - Wd Wd Wd & Wd Wd Wd - Wd Wd Wd d - E de
50 & d Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS Ext ext heat Consumers consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Sub-installation 1 Product benchmark Fuel Waste gases Heat Electricity ^ d d d ld & Wd ^ d - d d - / d Wd - d d ^ d - d Wd
51 & d Input fuel P1 (fall-back, exposed) P2 (benchmark), exposed Flare Non-ETS Ext ext heat Consumers consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Sub-installation 2 Heat benchmark, CL Fuel Waste gases Heat Electricity ^ d - d Wd Wd d^ - d Wd Wd d^ d ^ d d ^ d - ^ d Wd Wd - d d ^ d ^ d ^ d - d, > d Wd Wd
52 & d Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS Ext ext heat Consumers consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Fuel Sub-installation 3 Heat benchmark, non CL Waste gases Compressor Heat Electricity ^ d d ^ d - ^ d > / d^ d^ / d^ - d d ' e ^ d d ^ d ^ d d, > d d^
53 & d Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS ext heat Consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Sub-installation 4 Fuel benchmark Fuel Waste gases Heat Electricity ^ d - d Wd Wd > d ^ d ^ d - Z / ^ d ^ d - /, > d,> ' e
54 & e Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS ext heat Consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Sub-installation 5 Historical emissions Fuel Waste gases Heat Electricity ^ d - / Wd Wd - & d d d -, d Wd Wd ^ d ^ d Z - d K d - d - d - d ^ d ^ d d K d D/Eh^ E d & ' e
55 & e Input fuel P1 (fall-back, exposed) P2 (benchmark, exposed) Flare Non-ETS ext heat Consumers (not exposed) P3 (fall-back, exposed) Steam turbine 1 Ext elec consumers Steam gen H1 Steam turbine 2 Steam gen H2 Compressor Fuel Waste gases Heat Electricity d Z
Waste gases and process emissions sub-installation
hzkwekdd/^^/ke /ZdKZd 'EZ> >/D/KE / D ' e h d^ Waste gases and process emissions sub-installation & e^ d d / d d d d e d d / ^ e d d d d d d d d d d d d ^ de d ^ de d d d de d d d de d d d de d / d d ^
More informationhzkwekdd/^^/ke /ZdKZd 'EZ> >/Ddd/KE / D ' e h d^ dddd, & & dd dddd d
hzkwekdd/^^/ke /ZdKZd'EZ> >/D/KE /D 'e hd^,& & d d d / d dd ^' d dd /D' d dd h' d dd d dd ^ d de W d d, e dd,d^ e dd,d^d^ dd,d^d^ d, dd K dd,d^ de dd,d^ dd D dd D de d ^d: dd dd d ^ dd, dd, d d / dd ^'
More informationd ^dzd K DZ/ '^ ^ '^ K '^ / '^ / DZ/ W / ^ d Eled ^ d Eldd dd d e t d d e de ^ '^ de ddl '^
DZ/, ^ : ' t ' D ^ E > E / D, ^ : ' W > E/D, E/, dd Z d dde Dddeed ddee ddd ddd dede E /, D d ^dzd K DZ/ '^ ^ '^ K '^ / '^ / DZ/ W / ^ d Eled ^ d Eldd dd d e t d d e de ^ '^ de ddl '^ d d '^ t '^ d /EdZKhd/KE
More informationQuestion&Answers. 9 November 2011
hzkwekdd/^^/ke /ZdKZd 'EZ> >/Ddd/KE / D Question&Answers h d^ dddd 9 November 2011 This document has been developed building on the frequently asked questions to the Helpdesk for the Member States Competent
More informationANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6
ANWE EY P 1 P 2 d fx d fh z P 3 P 4 m, m, m, m, m, m P 6 d d P 7 m P 5 m m P 10 d P 8 P 9 h,,, d d,, h v P 11 P 12,, m, m, m,, dd P 13 m f m P 18 h m P 22 f fx f fh fm fd P 14 m h P 19 m v x h d m P 15
More informationPublished Ahead of Print on August 16, 2018, as doi: /haematol Copyright 2018 Ferrata Storti Foundation.
Published Ahead of Print on August 16, 2018, as doi:10.3324/haematol.2018.196121. Copyright 2018 Ferrata Storti Foundation. Computed tomography pulmonary angiography versus ventilation-perfusion lung scan
More informationR-CHOP 14 with or without radiotherapy in non-bulky limited-stage diffuse large B-cell lymphoma (DLBCL)
R-CHOP 14 with or without radiotherapy in non-bulky limited-stage diffuse large B-cell lymphoma (DLBCL) Thierry Lamy, Gandhi Damaj, Pierre Soubeyran, Emmanuel Gyan, Guillaume Cartron, Krimo Bouabdallah,
More information08257 ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6
P 1 P 2 d fx d fh z P 3 P 4 m, m, m, m, m, m P 6 d d P 7 m P 5 m m P 10 P 8 P 9 h,,, d d,, d v P 11 P 12,, m, m, m,, dd P 13 m f m P 18 h m P 22 f fx f fh fm fd P 14 m h P 19 m v x h d m P 15 m m P 20
More information1 The terms included in the question can be defined as follows:
^W /E^dZhd/KE^&KZd,Z^WKEEd^ d ^W ^W^ /W ^/W 'WW 'WW W&W& & KK& /^ Wd d K dd t d W& Wed D / / d dddd o z o E ^D o ' o ^ W t o o o & o d o o o, o o Z o o, o K o K W o W o D^ o / o o E o / o o K W W ^ d ^W
More informationCopyright 2010 by the American Society for Pharmacology and Experimental Therapeutics.
DMD This Fast article Forward. has not been Published copyedited and on formatted. July 15, The 2010 final as version doi:10.1124/dmd.110.033936 may differ from this version. / & W W, / > W > Z z d >,
More informationPublished Ahead of Print on July 9, 2015, as doi: /haematol Copyright 2015 Ferrata Storti Foundation.
Published Ahead of Print on July 9, 2015, as doi:10.3324/haematol.2015.125864. Copyright 2015 Ferrata Storti Foundation. Impact of prior treatment and depth of response on survival in MM-003, a randomized
More informationSET-Plan - SOLAR THERMAL ELECTRICITY EUROPEAN INDUSTRIAL INITIATIVE (STE-EII)
SET-Plan - SOLAR THERMAL ELECTRICITY EUROPEAN INDUSTRIAL INITIATIVE (STE-EII) IMPLEMENTATION PLAN 2013-2015 dd dddd ^//d d ^ / / ^d / dddd dddd /Ey /Ey d '>K^^Zz d /EdZKhd/KE e /,/sded^/ez ^/Ed,'/EE/E'K&d,^d
More informationW W D D ddd ^ D,, Z > tdddee d lddddddededdedd ' d W d
dd WZde de& WZddd ' d d d E < d K d ' ^ d Z d Z E ' d d >, d K D d K d Z E d > E d D e E ^ e W D D d d ^ D / > > h < d W D / W W E < > > h < d / / ^ > h < d Y ^ D ^ / E h > > h < d / > > h < e D ^ E h
More informationPrayer. Volume III, Issue 17 January 11, Martin Luther King Jr. Prayer. Assumption Catholic School 1
Vm III, I 17 J 11, 2017 TROJAN NEW W Rpb Cz, E Cmm, L L L, d A Ch wh bd mm d mk p. P M Lh K J. P Gd h h h Am d A h wd, W w h h hh w; w whh M w h bh. A w whh h h wd w B h wd pwh, Ad h p p hk. A w whh m
More informationh D t del d ddl ddl el del d < d
> Z Z d : d h D d, Z d d / d W < ^ d d d ' e W E e > ^ d d / & d e ^ < e Z d e & D d e h s d : ^ d e d ' D ' h ' ' ' d / / ' h ^ ^ ' d / / ' & ' h D ' ' ' d W ' h ' ' ' d ' D ' ' > ' h ' ' ' e D /' /EZh
More informationMediastinal Grey Zone Lymphoma: clinico-pathological characteristics and outcomes of 99 patients from the LYSA
Published Ahead of Print on October 6, 2016, as doi:10.3324/haematol.2016.152256. Copyright 2016 Ferrata Storti Foundation. Mediastinal Grey Zone Lymphoma: clinico-pathological characteristics and outcomes
More informationMusical Instruments. Answers
m w Wkh 1 m my Wdwd my g my my m m V m 3. W h m f h m h Y V,, D 4. W h m f h m h Y. h h, 5. W h m f h m h U Y Dm, g, 6. W h m f h m h WDWD Y,, 7. whh fmy d h XY g? Wkh 2 g my h fwg m g m. m m hk Whh g
More information3 Energy Exchange in Turbomachines
3 Energy Exchange in Turbomachines Problem 1 The solved and unsolved examples of this chapter are meant to illustrate the various forms of velocity triangles and the variety of the turbomachines. In addition,
More informationMolecular Pharmacology Fast Forward. Published on June 29, 2016 as DOI: /mol This article has not been copyedited and formatted.
, W D E / & h E D D D Z W, W D / & h dddd h D D d dddddedddede dddddeddddee & dddddedddede d d d & d dee d eddd Z dde DW d d d W/ d d e e d d d d d, d /^ d db d db E< E l
More informationLecture 35: Vapor power systems, Rankine cycle
ME 00 Thermodynamics I Spring 015 Lecture 35: Vapor power systems, Rankine cycle Yong Li Shanghai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Chuan Road Shanghai, 0040, P. R.
More informationWeek 5. Energy Analysis of Closed Systems. GENESYS Laboratory
Week 5. Energy Analysis of Closed Systems Objectives 1. Examine the moving boundary work or PdV work commonly encountered in reciprocating devices such as automotive engines and compressors 2. Identify
More informationAAE COMBUSTION AND THERMOCHEMISTRY
5. COMBUSTIO AD THERMOCHEMISTRY Ch5 1 Overview Definition & mathematical determination of chemical equilibrium, Definition/determination of adiabatic flame temperature, Prediction of composition and temperature
More informationMolecular Pharmacology Fast Forward. Published on January 6, 2017 as DOI: /mol This article has not been copyedited and formatted.
d/d>w' d zddd & Z d ' W d : z t Z ' :, & D W, > > d/w/ D^ Z / Dh^ d W zt Z' d D^ Z / Dh^ ' d: :, &D >> d/w/ D ^ ' W, d ZhEE/E'd/d>W' Z W D^ Z / ddd d Dddedd ld eee ded dddd d de E d E e E de ddd / edd
More informationSustainable Power Generation Applied Heat and Power Technology. Equations, diagrams and tables
Sustainable Power Generation Applied Heat and Power Technology Equations, diagrams and tables 1 STEAM CYCLE Enthalpy of liquid water h = c p,liquid (T T ref ) T ref = 273 K (normal conditions). The specific
More informationChapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 7 Entropy by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics: An Engineering Approach, 5th ed.,
More information1. What is the phenomenon that best explains why greenhouse gases absorb infrared radiation? D. Diffraction (Total 1 mark)
1. What is the phenomenon that best explains why greenhouse gases absorb infrared radiation? A. Resonance B. Interference C. Refraction D. Diffraction 2. In which of the following places will the albedo
More informationII/IV B.Tech (Regular) DEGREE EXAMINATION. (1X12 = 12 Marks) Answer ONE question from each unit.
Page 1 of 8 Hall Ticket Number: 14CH 404 II/IV B.Tech (Regular) DEGREE EXAMINATION June, 2016 Chemical Engineering Fourth Semester Engineering Thermodynamics Time: Three Hours Maximum : 60 Marks Answer
More informationCHAPTER 6 THE SECOND LAW OF THERMODYNAMICS
CHAPTER 6 THE SECOND LAW OF THERMODYNAMICS S. I. Abdel-Khalik (2014) 1 CHAPTER 6 -- The Second Law of Thermodynamics OUTCOME: Identify Valid (possible) Processes as those that satisfy both the first and
More informationNonverbal Cues of Dominance Laura van Hooff, Jasmijn Verspaandonk, Nicole van den Reek, Guusje Nagels & Jalou Lemmens
Nvbl C f Dm L v Hff, Jmj Vdk, Nl v d Rk, Gj Nl & Jl Lmm Ab Th m f h d w v h vbl x f dm b hm d whh h w dff bw l d dm T h, h l bhv f f h TV hw Tm Ild w ld Th x vbl bhvl d h h m dm w d, h, l x, fld m, hd
More informationc Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)
Thermodynamic Processes & Isentropic Efficiency Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-1000, Bangladesh zahurul@me.buet.ac.bd
More informationHistorical review of glasses used for parenteral packaging
Downloaded from on November 13, 2018 Historical review of glasses used for parenteral packaging Robert A Schaut and W. Porter Weeks PDA Journal of Pharmaceutical Science and Technology 2017, Access the
More informationCONSUMER GRIEVANCE REDRESSAL FORUM K OLHAPUR P hones : & K olhapur Zone, nd Vidyut Bhavan, 2 f loor, Fax No T araba
ONUMER GREVANE REDREAL FORUM K OLAPUR P h : 021-2666001 & K lh Z, 2666002 Vdy Bhv, 2 l, Fx 021-2666001 Pk, K lh 416 00 -ml- klh@mhdm m 171/12-1/ 122 D : 28201 J UDGMEN 1 ) Y hw hk Gl Kkh, ( 171/ 121) dhw
More informationApplied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur
Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 8 Introduction to Vapour Power Cycle Today, we will continue
More informationPARTICULATES #1. Introduction
Introduction PARTICULATES #1 Ash-forming elements in fuels Particulate emission standards Options for particulate control emissions Gravity settlers Gas cyclones Electrostatic precipitators see: www.hut.fi/~rzevenho/gasbook
More informationApplied Chemical Processes - S Energy in chemicall processes. Types of energy 3/5/2013
3/5/03 Applied Chemical Processes - S0500 Sylabus. Design of chemical technology. Treatment and mass transfer in chemical processes 3. Energy in chemical processes 4. Separation processes 5. Kinetics of
More information7. Development of the 2nd Law
7-1 7. Development of the 2nd Law 7.1 1st Law Limitations The 1 st Law describes energy accounting. Once we have a process (or string of processes) we can calculate the relevant energy interactions. The
More informationIn the name of Allah
In the name of Allah Physical chemistry- 2 nd state semester 1 Petroleum and petrochemical engineering. Lecture No. 5,6 Thermodynamics 6-11-2016 27-11-2016 Assistance prof. Dr. Luma Majeed Ahmed lumamajeed2013@gmail.com,
More informationMAE 320 HW 7B. 1e. For an isolated system, please circle the parameter which will change with time. (a) Total energy;
MAE 320 HW 7B his comprehensive homework is due Monday, December 5 th, 206. Each problem is worth the points indicated. Copying of the solution from another is not acceptable. Multi-choice, multi-answer
More informationApplied chemical processes Energy in chemicall processes. Types of energy. Overall energy balance
Applied chemical processes Energy in chemicall processes types of energy overall energy balance heat balance cooling and heating in chemical proc. electrical energy Types of energy Energy in chemical processes
More information98 Series Backpressure Regulators and Relief Valves
9 Series Backpressure Regulators and Relief Valves Bulletin.:9 November 09 W TYPE 9H W TYPE 9LD Figure. Typical 9 Relief Valves Introduction W TYPE 9HD The 9 Series (Figure ) is used for backpressure or
More informationSEM-2017(03HI MECHANICAL ENGINEERING. Paper II. Please read each of the following instructions carefully before attempting questions.
We RoU No. 700095 Candidate should write his/her Roll No. here. Total No. of Questions : 7 No. of Printed Pages : 7 SEM-2017(03HI MECHANICAL ENGINEERING Paper II Time ; 3 Hours ] [ Total Marks : 0 Instructions
More informationEngineering Thermodynamics Solutions Manual
Engineering Thermodynamics Solutions Manual Prof. T.T. Al-Shemmeri Download free books at Prof. T.T. Al-Shemmeri Engineering Thermodynamics Solutions Manual 2 2012 Prof. T.T. Al-Shemmeri & bookboon.com
More informationSpring_#8. Thermodynamics. Youngsuk Nam
Spring_#8 Thermodynamics Youngsuk Nam ysnam1@khu.ac.krac kr Ch.7: Entropy Apply the second law of thermodynamics to processes. Define a new property called entropy to quantify the secondlaw effects. Establish
More informationCustomer-Meter Unit Cost of Electricity Customer-Meter Unit Cost of Electricity ($/kwh) = [Total Cost ($/yr) - Option Capacity Value ($/yr)]
Customer-Meter Unit Cost of Electricity Customer-Meter Unit Cost of Electricity ($/kwh) = [Total Cost ($/yr) - Option Capacity Value ($/yr)] Equivalent Capacity (MW)*1000*8760 Total Cost ($/yr) = Nominal
More informationDistinguish between. and non-thermal energy sources.
Distinguish between System & Surroundings We also distinguish between thermal We also distinguish between thermal and non-thermal energy sources. P Work The gas in the cylinder is the system How much work
More informationSECOND ENGINEER REG. III/2 APPLIED HEAT
SECOND ENGINEER REG. III/2 APPLIED HEAT LIST OF TOPICS A B C D E F G H I J K Pressure, Temperature, Energy Heat Transfer Internal Energy, Thermodynamic systems. First Law of Thermodynamics Gas Laws, Displacement
More informationChapter 7. Entropy: A Measure of Disorder
Chapter 7 Entropy: A Measure of Disorder Entropy and the Clausius Inequality The second law of thermodynamics leads to the definition of a new property called entropy, a quantitative measure of microscopic
More informationAppendix 4. Appendix 4A Heat Capacity of Ideal Gases
Appendix 4 W-143 Appendix 4A Heat Capacity of Ideal Gases We can determine the heat capacity from the energy content of materials as a function of temperature. The simplest material to model is an ideal
More informationMrs Linda Everard, BSc. The Early Intervention Service. 1 Miller Street. Aston. Birmingham B6 4NF.
1 Dr Anna Lavis, MA MSc MRes PhD. School of Health and Population Sciences, University of Birmingham. Primary Care Clinical Sciences Building. Edgbaston. Birmingham B15 2TT. Email: a.c.lavis@bham.ac.uk
More informationEntropy balance special forms. Quasiequilibrium (QE) process. QE process is reversible. dt Tk = = +
Entropy balance Outline Closed systems Open systems Reversible steady flow wor Minimizing compressor wor Isentropic efficiencies Examples Entropy balance Sin Sout + Sgen = Ssys Entropy balance Entropy
More informationWhere F1 is the force and dl1 is the infinitesimal displacement, but F1 = p1a1
In order to force the fluid to flow across the boundary of the system against a pressure p1, work is done on the boundary of the system. The amount of work done is dw = - F1.dl1, Where F1 is the force
More information8.21 The Physics of Energy Fall 2009
MIT OpenCourseWare http://ocw.mit.edu 8.21 The Physics of Energy Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.21 Lecture 9 Heat Engines
More informationEntropy and the Second Law of Thermodynamics
Entropy and the Second Law of Thermodynamics Reading Problems 7-1 7-3 7-88, 7-131, 7-135 7-6 7-10 8-24, 8-44, 8-46, 8-60, 8-73, 8-99, 8-128, 8-132, 8-1 8-10, 8-13 8-135, 8-148, 8-152, 8-166, 8-168, 8-189
More informationEarlier Topics. Introduction to Cryogenic Engineering An introductory knowledge of Cryogenic Engineering.
8 1 Earlier Topics Introduction to Cryogenic Engineering An introductory knowledge of Cryogenic Engineering. Properties of Cryogenic Fluids Properties of Cryogens, T s diagram, Hydrogen, Helium. Properties
More informationMAE 11. Homework 8: Solutions 11/30/2018
MAE 11 Homework 8: Solutions 11/30/2018 MAE 11 Fall 2018 HW #8 Due: Friday, November 30 (beginning of class at 12:00p) Requirements:: Include T s diagram for all cycles. Also include p v diagrams for Ch
More informationChair Susan Pilkington called the meeting to order.
PGE PRK D RECREO DVOR COMMEE REGUR MEEG MUE MOD, JU, Ru M h P P d R d Cmm hd : m Ju,, h Cu Chmb C H P, z Ch u P dd, Mmb B C, Gm Cu D W Bd mmb b: m D, d Md z ud mmb : C M, J C P Cmmu Dm D, Km Jh Pub W M,
More informationand mol of Cl 2 was heated in a vessel of fixed volume to a constant temperature, the following reaction reached equilibrium.
Q1. When a mixture of 0.45 mol of PCl and 0.68 mol of Cl was heated in a vessel of fixed volume to a constant temperature, the following reaction reached equilibrium. PCl + Cl PCl 5 H = 9 kj mol 1 At equilibrium,
More informationName: Applied Physics II Exam 2 Winter Multiple Choice ( 8 Points Each ):
Name: e-mail: Applied Physics II Exam 2 Winter 2006-2007 Multiple Choice ( 8 Points Each ): 1. A cowboy fires a silver bullet ( specific heat c = 234 J / kg O C ) with a muzzle speed of 200 m/s into a
More informationLecture 43: Aircraft Propulsion
Lecture 43: Aircraft Propulsion Turbojet Engine: 1 3 4 fuel in air in exhaust gases Diffuser Compressor Combustor Turbine Nozzle 43.1 T Ideal Ccle: w T,s = w C,s s 1 s w T,s w C,s 3 4 s s Processes: 1:
More informationTurbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics.
Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics. F. Ravelet Laboratoire DynFluid, Arts et Metiers-ParisTech February 3, 2016 Control volume Global balance equations in open systems
More informationDistributed quasi-newton method and its application to the optimal reactive power flow problem
1 Distributed quasi-newton method and its application to the optimal reactive power flow problem Saverio Bolognani Power distribution networks 2 Transmission Grid Distribution Grid up to ~150 MW Rural
More informationLecture 44: Review Thermodynamics I
ME 00 Thermodynamics I Lecture 44: Review Thermodynamics I Yong Li Shanghai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Chuan Road Shanghai, 0040, P. R. China Email : liyo@sjtu.edu.cn
More informationSTATE OF FLORIDA DEPARTMENT OF TRANSPORTATION CONTRACT PLANS FINANCIAL PROJECT ID
LD M L HL LLG M L LLH DM L KVLL WL H LK M G GVLL L L D H DLD LD L L D --- W H G - D D (-) D L H ML LKLD D W K M M () K H H M HL L DLD D H H D W LM H M L w Hmmc -- y L D u x p, HL Hu w x DG # G p Mm G um
More informationE11 Lecture 8: Fuel Cell Power and Energy Conservation. Professor Lape Fall 2010
E11 Lecture 8: Fuel Cell Power and Energy Conservation Professor Lape Fall 2010 Overview How much power can your FC produce? Maximum power Polarization curve How can we convert this power to other forms
More informationParts Manual. EPIC II Critical Care Bed REF 2031
EPIC II Critical Care Bed REF 2031 Parts Manual For parts or technical assistance call: USA: 1-800-327-0770 2013/05 B.0 2031-109-006 REV B www.stryker.com Table of Contents English Product Labels... 4
More informationLecture 37. Heat of Reaction. 1 st Law Analysis of Combustion Systems
Department of Mechanical Engineering ME 322 Mechanical Engineering hermodynamics Heat of eaction Lecture 37 1 st Law Analysis of Combustion Systems Combustion System Analysis Consider the complete combustion
More informationFundamentals of Thermodynamics. Chapter 8. Exergy
Fundamentals of Thermodynamics Chapter 8 Exergy Exergy Availability, available energy Anergy Unavailable energy Irreversible energy, reversible work, and irreversibility Exergy analysis : Pure Thermodynamics
More informationFirst Law of Thermodynamics
CH2303 Chemical Engineering Thermodynamics I Unit II First Law of Thermodynamics Dr. M. Subramanian 07-July-2011 Associate Professor Department of Chemical Engineering Sri Sivasubramaniya Nadar College
More informationIntroduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303
Introduction to Chemical Engineering Thermodynamics Chapter 7 1 Thermodynamics of flow is based on mass, energy and entropy balances Fluid mechanics encompasses the above balances and conservation of momentum
More information"Thermodynamic Analysis of Processes for Hydrogen Generation by Decomposition of Water"
"Thermodynamic Analysis of Processes for Hydrogen Generation by Decomposition of Water" by John P. O'Connell Department of Chemical Engineering University of Virginia Charlottesville, VA 22904-4741 A Set
More informationAtmospheric Analysis Gases. Sampling and analysis of gaseous compounds
Atmospheric Analysis Gases Sampling and analysis of gaseous compounds Introduction - External environment (ambient air) ; global warming, acid rain, introduction of pollutants, etc - Internal environment
More informationLet a system undergo changes from a state 1 to state 2.
ME 410 Day 11 Topics First Law of Thermodynamics Applied to Combustion Constant olume Combustion Constant ressure Combustion Enthalpy of Formation Heating alues of Fuels 1. The First Law of Thermodynamics
More informationEnthalpy and Adiabatic Changes
Enthalpy and Adiabatic Changes Chapter 2 of Atkins: The First Law: Concepts Sections 2.5-2.6 of Atkins (7th & 8th editions) Enthalpy Definition of Enthalpy Measurement of Enthalpy Variation of Enthalpy
More informationUNIT I Basic concepts and Work & Heat Transfer
SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code: Engineering Thermodynamics (16ME307) Year & Sem: II-B. Tech & II-Sem
More informationToday lecture. 1. Entropy change in an isolated system 2. Exergy
Today lecture 1. Entropy change in an isolated system. Exergy - What is exergy? - Reversible Work & Irreversibility - Second-Law Efficiency - Exergy change of a system For a fixed mass For a flow stream
More informationThermodynamics II. Week 9
hermodynamics II Week 9 Example Oxygen gas in a piston cylinder at 300K, 00 kpa with volume o. m 3 is compressed in a reversible adiabatic process to a final temperature of 700K. Find the final pressure
More information3. First Law of Thermodynamics and Energy Equation
3. First Law of Thermodynamics and Energy Equation 3. The First Law of Thermodynamics for a ontrol Mass Undergoing a ycle The first law for a control mass undergoing a cycle can be written as Q W Q net(cycle)
More informationOutline. Property diagrams involving entropy. Heat transfer for internally reversible process
Outline roperty diagrams involving entropy What is entropy? T-ds relations Entropy change of substances ure substances (near wet dome) Solids and liquids Ideal gases roperty diagrams involving entropy
More information열과유체, 에너지와친해지기 KAIST 기계공학과정상권
열과유체, 에너지와친해지기 KAIST 기계공학과정상권 이번시간에는! 열역학 - 세상을움직이는스마트한법칙 물과공기로움직이는기계 사라지지않는에너지 / 증가하는엔트로피 열역학 - 세상을움직이는스마트한법칙 KAIST 기계공학과정상권 [ 학습목차 ] Thermofluids Energy conservation principle Energy Work (boundary work)
More informationJet Aircraft Propulsion Prof. Bhaskar Roy Prof. A.M. Pradeep Department of Aerospace Engineering
Jet Aircraft Propulsion Prof. Bhaskar Roy Prof. A.M. Pradeep Department of Aerospace Engineering Indian Institute of Technology, IIT Bombay Module No. # 01 Lecture No. # 08 Cycle Components and Component
More informationCAT. NO /irtl,417~ S- ~ I ';, A RIDER PUBLICATION BY H. A. MIDDLETON
CAT. NO. 139-3 THIRD SUPPLEMENT I /irtl,417~ S- ~ I ';,... 0 f? BY H. A. MIDDLETON.. A RIDER PUBLICATION B36 B65 B152 B309 B319 B329 B719 D63 D77 D152 DA90 DAC32 DAF96 DC70 DC80 DCC90 DD6 DD7 DF62 DF91
More informationBlood First Edition Paper, prepublished online March 7, 2018; DOI /blood
Blood First Edition Paper, prepublished online March 7, 2018; DOI 10.1182/blood-2017-12-822817 ^ E& /s>> > >zdw,k/ekw>^/, Dzee ee D Z ^ d W D : d Z t d D, s d D : d ^ & ^ d :,, s d Z d t < d D : < d D
More informationContents. 2 Basic Components Aerofoils Force Generation Performance Parameters xvii
Contents 1 Working Principles... 1 1.1 Definition of a Turbomachine... 1 1.2 Examples of Axial Turbomachines... 2 1.2.1 Axial Hydraulic Turbine... 2 1.2.2 Axial Pump... 4 1.3 Mean Line Analysis... 5 1.4
More informationSection 4.1: Introduction to Jet Propulsion. MAE Propulsion Systems II
Section 4.1: Introduction to Jet Propulsion Jet Propulsion Basics Squeeze Bang Blow Suck Credit: USAF Test Pilot School 2 Basic Types of Jet Engines Ramjet High Speed, Supersonic Propulsion, Passive Compression/Expansion
More informationModeling and Analysis of Dynamic Systems
Modeling and Analysis of Dynamic Systems Dr. Guillaume Ducard Fall 2017 Institute for Dynamic Systems and Control ETH Zurich, Switzerland G. Ducard c 1 / 34 Outline 1 Lecture 7: Recall on Thermodynamics
More informationalkane molecular formula boiling point / C H 6 H 8 H [1] Explain why the boiling points increase down the alkane homologous series....
1 The alkanes are an homologous series of hydrocarbons. The table shows information about some straight chain alkanes. alkane molecular formula boiling point / methane 4 164 ethane 2 6 89 propane 3 8 42
More informationSpring_#7. Thermodynamics. Youngsuk Nam.
Spring_#7 Thermodynamics Youngsuk Nam ysnam1@khu.ac.kr You can t connect the dots looking forward; you can only connect them looking backwards. So you have to trust that the dots will somehow connect in
More informationHeat Integration - Introduction
Heat Integration - Introduction Sub-Topics Design of Heat Exchanger Networks Selection of Utilities Ø Consumption and Production Correct Integration Ø Distillation and Evaporation Ø Heat Pumps Ø Turbines
More informationChemical Engineering Thermodynamics
Chemical Engineering Thermodynamics P Liquid P x 1 sat P 1 T sat T 2 T x 1 T x 1 T y 1 Liquid Vapour sat P 2 P x 1 P y 1 P y 1 Vapour sat T 1 x, y 1 1 x, y 1 1 Pradeep Ahuja Contents CHEMICAL ENGINEERING
More informationThermal Energy Final Exam Fall 2002
16.050 Thermal Energy Final Exam Fall 2002 Do all eight problems. All problems count the same. 1. A system undergoes a reversible cycle while exchanging heat with three thermal reservoirs, as shown below.
More informationTurbomachinery. Hasan Ozcan Assistant Professor. Mechanical Engineering Department Faculty of Engineering Karabuk University
Turbomachinery Hasan Ozcan Assistant Professor Mechanical Engineering Department Faculty of Engineering Karabuk University Introduction Hasan Ozcan, Ph.D, (Assistant Professor) B.Sc :Erciyes University,
More informationExam Stochastic Processes 2WB08 - March 10, 2009,
Exam Stochastic Processes WB8 - March, 9, 4.-7. The number of points that can be obtained per exercise is mentioned between square brackets. The maximum number of points is 4. Good luck!!. (a) [ pts.]
More informationPublished Ahead of Print on August 1, 2014, as doi: /haematol Copyright 2014 Ferrata Storti Foundation.
Published Ahead of Print on August 1, 2014, as doi:10.3324/haematol.2014.106096. Copyright 2014 Ferrata Storti Foundation. Outcome of Aplastic Anemia in adolescence. A survey of the Severe Aplastic Anemia
More informationCourse: MECH-341 Thermodynamics II Semester: Fall 2006
FINAL EXAM Date: Thursday, December 21, 2006, 9 am 12 am Examiner: Prof. E. Timofeev Associate Examiner: Prof. D. Frost READ CAREFULLY BEFORE YOU PROCEED: Course: MECH-341 Thermodynamics II Semester: Fall
More informationHydraulic modeling assessment Copyright 2010, Optimized Technical Solutions, LLC
Hydraulic modeling assessment Copyright 2010, Optimized Technical Solutions, LLC Name: Date: Please answer the following questions with the complete piping configuration shown in Figure 1 below. Assume
More informationIN HIS PRESENCE UNITE YOUR PRAYERS WITH THE PRAYERS OF JESUS
IN HIS PRESENCE UNITE YOUR PRAYERS WITH THE PRAYERS OF ESUS 9 I p m m 10 A I d m Ad m m m 11 H F p m b pw m m m m b w 14 I m wd d wd d m wd m I m wd 15 M p m wd b p m m 16 T wd I m 17 S m b ; wd 18 A m
More informationSPH 302 THERMODYNAMICS
THERMODYNAMICS Nyongesa F. W., PhD. e-mail: fnyongesa@uonbi.ac.ke 1 Objectives Explain the Laws of thermodynamics & their significance Apply laws of thermodynamics to solve problems relating to energy
More informationER100/200, Pub Pol 184/284 Energy Toolkit III:
ER100/200, Pub Pol 184/284 Energy Toolkit III: Energy Thermodynamics Lectures 6 & 7 9-15 & 17-2015 Outline What can the energy analyst do with Thermodynamics? 1 st Law of Thermodynamics 2 nd Law of Thermodynamics
More informationInternational ejournals
Available online at www.internationalejournals.com International ejournals International ejournal of Mathematics and Engineering 170 (2012) 1603 1612 Design and Coupled Field Analysis of First Stage Gas
More information05/04/2011 Tarik Al-Shemmeri 2
05/04/2011 Tarik Al-Shemmeri 1 05/04/2011 Tarik Al-Shemmeri 2 05/04/2011 Tarik Al-Shemmeri 3 05/04/2011 Tarik Al-Shemmeri 4 05/04/2011 Tarik Al-Shemmeri 5 05/04/2011 Tarik Al-Shemmeri 6 05/04/2011 Tarik
More information