CE 374 K Hydrology. Evaporation. Daene C. McKinney
|
|
- Brianne Lamb
- 6 years ago
- Views:
Transcription
1 C 374 Hydrology aporation Daene C. Mcinney
2 aporation Terminology aporation: liquid ater pae directly to the apor phae Tranpiration: liquid ater pae from liquid to apor through plant metabolim Sublimation: ater pae directly from the olid phae to the apor phae
3 Factor Influencing aporation nergy upply for aporization (latent heat) Solar radiation Tranport of apor aay from eaporatie urface Wind elocity oer urface Specific humidity gradient aboe urface Vegetated urface Supply of moiture to the urface apotranpiration (T) Potential apotranpiration (PT) moiture upply i not limited
4 aporation from a Water Surface Senible heat to air H Net radiation R n Vapor flo rate m& ρ A ρ a National Weather Serice Cla A type Intalled on a ooden platform in a gray location Filled ith ater to ithin.5 inche of the top aporation rate i meaured by manual reading or ith an analog output eaporation gauge CS dh Area, A ρ G Heat conducted to ground h
5 Method of timating aporation nergy method Aerodynamic method Combined method
6 nergy Method Continuity of Liquid Phae H R n m& ρ a m& d ρ d + CV ρ V CS da dh ρ G h dh ρ A dh 0 No flo of liquid ater through CS m& ρ A
7 nergy Method () Vapor Phae - Continuity m& d q ρ d + CV a q CS ρ V a da H R n m& 0 ρ a m& q CS ρ V da a ρ A Steady flo of air oer ater dh ρ h ρ A q CS ρ V a da G ρ A q CS ρ V a da
8 nergy Method (3) nergy q. H R n m& dh 0 dw d ( e + ( e + V / + gz) ρd CV u u + V / + gz) ρv r d CS A r 0; V 0, h cont. dh ρ a ρ h dh d e u ρ d CV R n H G G dh R n H G
9 nergy Method (4) nergy q. for Water in CV dh Rn H G Aume:. Contant temp of ater in CV. Change of heat i change in internal energy of eaporated ater dh l m & H R n dh m& ρ a ρ G h l m& R n H G Recall: m& ρ A l ρ A ( R H G) n r Rn l ρ Neglecting enible and ground heat fluxe
10 Aerodynamic Method Include tranport of apor aay from ater urface a function of: Humidity gradient aboe urface Wind peed acro urface Upard apor flux dq q m& ρ a ρa dz z Upard momentum flux du τ ρam ρam dz u z u z q z m& τ R n Air Flo aporation Net radiation ( q q ) m ( u u )
11 m& Aerodynamic Method () τ ( q q ) m ( u u ) R n Net radiation Log-elocity profile u τ ρ a Z ln k Z Momentum flux m& τ k ρ a ρ k ln a m o ( u u ) ( Z Z ) ( q q )( ) u u [ ln( Z Z )] Thornthaite-Holzman quation Air Flo aporation Too many ariable! Often only kno q and u at eleation
12 Aerodynamic Method (3) Simplify R n Net radiation a B ( e e) B Pρ 0.6k ρ u [ ln( Z Z )] a o Air Flo aporation e apor preure e at. apor preure
13 Combined Method aporation could be calculated by Aerodynamic method: hen energy upply i not limiting nergy method: hen apor tranport i not limiting Normally, both are limiting, o ue a combination method
14 Combined Method (Cont.) Combining nergy balance Aerodynamic Method Combined Method Δ γ r + a Δ + γ Δ + γ γ C p r 0.6l R n l ρ a h p B ( e e) 4098e Δ ( T ) Well uited to mall area ith detailed data Net Radiation Air Temperature Humidity Wind Speed Air Preure. 3 Δ Δ + γ r Prietly & Taylor
15 xample Ue Combo Method to find aporation z m P 0.3 kpa u 3 m/ R n 00 W/m T 5 degc R h 40% l r.50x T (500.36*5) x0 R 00 n l ρ x * mm/day 3 44 kj/kg
16 xample (Cont.) Ue Combo Method to find aporation z m P 0.3 kpa u 3 m/ R n 00 W/m T 5 degc 0.6k ρ u 0.6*0.4 *.9*3 4.54x0 RB h 40% a Pρ [ ln( )] ( 4 ) Z Zo 0.3*997 ln 3x0 e e 367Pa R h * e 0.4* Pa [ ] m/pa a 4.54x0 7.45mm/day ( ) *(000 mm /m)*(86400 /day)
17 xample (Cont.) Ue Combo Method to find aporation z m P 0.3 kpa u 3 m/ R n 00 W/m T 5 degc R h 40% C ph p 005*0.3x0 γ 0.6l 3 0.6* 44x0 4098e Δ ( T ) Δ Δ + γ *367 ( ) 3 γ 0.6 Δ + γ 67.Pa/degC 88.7 Pa/degC Δ γ r + Δ + γ Δ + γ a 0.738* * mm/day
18 xample Ue Prietly-Taylor Method to find aporation rate for a ater body z m P 0.3 kpa u 3 m/ R n 00 W/m T 5 degc R h 40%. 3 Δ Δ + γ r Prietly & Taylor Δ r 7.0 mm/day Δ + γ.3*0.738* mm/day
19 apotranpiration apotranpiration Combination of eaporation from oil urface and tranpiration from egetation Goerning factor nergy upply and apor tranport Supply of moiture at eaporatie urface Reference crop 8-5 cm of healthy groing green gra ith abundant ater Combo Method ork ell if B i calibrated to local condition
20 Potential apotranpiration Multiply reference crop T by a Crop Coefficient and a Soil Coefficient T Actual T T r Reference Crop T k c Crop Coefficient; 0. k k 0 k c T k.3 Soil Coefficient; k c T r Crop Coefficient, kc CORN Time Since Planting (Day)
21
22 Combined Method aporation could be calculated by Aerodynamic method: hen energy upply i not limiting nergy method: hen apor tranport i not limiting Normally, both are limiting, o ue a combination method Senible heat flux i difficult to etimate ( ) Aume it i proportional to the apor heat flux H β lm& Where β Boen ratio nergy balance equation (G0) Rn H G lρ A R l m& + β n ( ) ( )
23 Combined Method () Tranport equation for heat and apor dz dq H ρ a dz dt C m h p ρ a & ( ) ) ( h p q q T T C m H & ( ) ) (.6 0 e e l T T p C h p β ( ) m l H & β p e q 6 0. h p l p C 0.6 γ ( ) ( ) e e T T γ β h
24 Recall Vapor Preure Vapor Preure R h e e Saturate apor preure for gien temperature e e Saturation Vapor Preure Vapor Preure De Point temp, Td Meaured temp, T Temperature 7.7T e 6exp T Δ de dt 4098e ( T )
Bernoulli s equation may be developed as a special form of the momentum or energy equation.
BERNOULLI S EQUATION Bernoulli equation may be developed a a pecial form of the momentum or energy equation. Here, we will develop it a pecial cae of momentum equation. Conider a teady incompreible flow
More informationEVAPORATION GEOG 405. Tom Giambelluca
EVAPORATION GEOG 405 Tom Giambelluca 1 Evaporation The change of phase of water from liquid to gas; the net vertical transport of water vapor from the surface to the atmosphere. 2 Definitions Evaporation:
More informationEvapotranspiration. Rabi H. Mohtar ABE 325
Evapotranspiration Rabi H. Mohtar ABE 325 Introduction What is it? Factors affecting it? Why we need to estimate it? Latent heat of vaporization: Liquid gas o Energy needed o Cooling process Saturation
More informationGreenhouse Steady State Energy Balance Model
Greenhouse Steady State Energy Balance Model The energy balance for the greenhouse was obtained by applying energy conservation to the greenhouse system as a control volume and identifying the energy terms.
More informationChapter 3 First Law of Thermodynamics and Energy Equation
Fundamentals of Thermodynamics Chapter 3 First Law of Thermodynamics and Energy Equation Prof. Siyoung Jeong Thermodynamics I MEE0-0 Spring 04 Thermal Engineering Lab. 3. The energy equation Thermal Engineering
More informationESCI 485 Air/Sea Interaction Lesson 1 Stresses and Fluxes Dr. DeCaria
ESCI 485 Air/Sea Interaction Lesson 1 Stresses and Fluxes Dr DeCaria References: An Introduction to Dynamic Meteorology, Holton MOMENTUM EQUATIONS The momentum equations governing the ocean or atmosphere
More informationChapter 12 Radiation Heat Transfer. Special Topic: Heat Transfer from the Human Body
Chapter 1 Radiation Heat ranfer Special opic: Heat ranfer from the Human Body 1-7C Ye, roughly one-third of the metabolic heat generated by a peron who i reting or doing light work i diipated to the environment
More information4.1 LAWS OF MECHANICS - Review
4.1 LAWS OF MECHANICS - Review Ch4 9 SYSTEM System: Moving Fluid Definitions: System is defined as an arbitrary quantity of mass of fixed identity. Surrounding is everything external to this system. Boundary
More informationEric. W. Harmsen 1, John Mecikalski 2, Vanessa Acaron 3 and Jayson Maldonado 3
Estimating Ground-Level Solar Radiation and Evapotranspiration In Puerto Rico Using Satellite Remote Sensing Eric. W. Harmsen 1, John Mecikalski 2, Vanessa Acaron 3 and Jayson Maldonado 3 1 Department
More informationSpring Semester 2011 March 1, 2011
METR 130: Lecture 3 - Atmospheric Surface Layer (SL - Neutral Stratification (Log-law wind profile - Stable/Unstable Stratification (Monin-Obukhov Similarity Theory Spring Semester 011 March 1, 011 Reading
More informationProblem 1 The turbine is an open system. We identify the steam contained the turbine as the control volume. dt + + =
ME Fall 8 HW olution Problem he turbe i an open ytem. We identiy the team contaed the turbe a the control volume. Ma conervation: t law o thermodynamic: Aumption: dm m m m dt + + de V V V m h + + gz +
More informationRadiation Heat Transfer
CM30 ranport I Part II: Heat ranfer Radiation Heat ranfer Profeor Faith Morrion Department of Chemical Engineering Michigan echnological Univerity CM30 ranport Procee and Unit Operation I Part : Heat ranfer
More informationTropical Cyclones: Steady State Physics
Tropical Cyclones: Steady State Physics Energy Production Carnot Theorem: Maximum efficiency results from a particular energy cycle: Isothermal expansion Adiabatic expansion Isothermal compression Adiabatic
More informationMETRIC tm. Mapping Evapotranspiration at high Resolution with Internalized Calibration. Shifa Dinesh
METRIC tm Mapping Evapotranspiration at high Resolution with Internalized Calibration Shifa Dinesh Outline Introduction Background of METRIC tm Surface Energy Balance Image Processing Estimation of Energy
More informationTypes of Heat Transfer
Type of Heat Tranfer Dv Dt x = k dt dx v T S 2 * * ( v GrT * z = + z H vap lat uject in the coure conduction (Fourier Law forced convection (due to flow ource term free convection (fluid motion due to
More informationAtmospheric Sciences 321. Science of Climate. Lecture 14: Surface Energy Balance Chapter 4
Atmospheric Sciences 321 Science of Climate Lecture 14: Surface Energy Balance Chapter 4 Community Business Check the assignments HW #4 due Today, HW#5 is posted Quiz Today on Chapter 3, too. Mid Term
More informationExternal Flows. Dye streak. turbulent. laminar transition
Eternal Flos An internal flo is surrounded by solid boundaries that can restrict the development of its boundary layer, for eample, a pipe flo. An eternal flo, on the other hand, are flos over bodies immersed
More information1 Introduction to Governing Equations 2 1a Methodology... 2
Contents 1 Introduction to Governing Equations 2 1a Methodology............................ 2 2 Equation of State 2 2a Mean and Turbulent Parts...................... 3 2b Reynolds Averaging.........................
More informationSnow Parameter Caused Uncertainty of Predicted Snow Metamorphism Processes
Sno Parameter Caused Uncertainty of Predicted Sno Metamorphism Processes Report on the Research Performed during the REU Program at the University of Alaska Fairbanks, Geophysical Institute, 903 Koyukuk
More informationThermodynamics Introduction and Basic Concepts
Thermodynamics Introduction and Basic Concepts by Asst. Prof. Channarong Asavatesanupap Mechanical Engineering Department Faculty of Engineering Thammasat University 2 What is Thermodynamics? Thermodynamics
More information1. Heterogeneous Systems and Chemical Equilibrium
1. Heterogeneous Systems and Chemical Equilibrium The preceding section involved only single phase systems. For it to be in thermodynamic equilibrium, a homogeneous system must be in thermal equilibrium
More informationUNITS FOR THERMOMECHANICS
UNITS FOR THERMOMECHANICS 1. Conitent Unit. Every calculation require a conitent et of unit. Hitorically, one et of unit wa ued for mechanic and an apparently unrelated et of unit wa ued for heat. For
More informationA GROUND-BASED PROCEDURE FOR ESTIMATING LATENT HEAT ENERGY FLUXES 1 Eric Harmsen 2, Richard Díaz 3 and Javier Chaparro 3
A GROUND-BASED PROCEDURE FOR ESTIMATING LATENT HEAT ENERGY FLUXES 1 Eric Harmsen 2, Richard Díaz 3 and Javier Chaparro 3 1. This material is based on research supported by NOAA-CREST and NASA-EPSCoR (NCC5-595).
More informationThe Study of Inverted V-Type Heat Pipe Cooling Mechanism Based on High Heat Flux Heating Elements
th IHPS, Taipei, Taian, No. 6-9, The Study of Inerted V-Type Heat Pipe Cooling Mechanism Based on High Heat Flux Heating Elements Li Jing, Ji Shengtao, Yao Zemin The Key Lab of Enhanced Heat Transfer and
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 informationRadiation in energy balance models. 1. A hierarchy of climate models. Lecture 25
Lecture 5 Radiation in energy balance model Objective: 1. A hierarchy of climate model.. Example of imple energy balance model. Required reading: L0: 8.5 1. A hierarchy of climate model. Climate model
More information( ) = 1005 J kg 1 K 1 ;
Problem Set 3 1. A parcel of water is added to the ocean surface that is denser (heavier) than any of the waters in the ocean. Suppose the parcel sinks to the ocean bottom; estimate the change in temperature
More informationRadiation, Sensible Heat Flux and Evapotranspiration
Radiation, Sensible Heat Flux and Evapotranspiration Climatological and hydrological field work Figure 1: Estimate of the Earth s annual and global mean energy balance. Over the long term, the incoming
More informationENT 254: Applied Thermodynamics
ENT 54: Applied Thermodynamics Mr. Azizul bin Mohamad Mechanical Engineering Program School of Mechatronic Engineering Universiti Malaysia Perlis (UniMAP) azizul@unimap.edu.my 019-4747351 04-9798679 Chapter
More informationA) At each point along the pipe, the volume of fluid passing by is given by dv dt = Av, thus, the two velocities are: v n. + ρgy 1
1) The horizontal pipe hon in Fig. 1 ha a diameter of 4.8 cm at the ider portion and 3.7 cm at the contriction. Water i floing in the pipe and the dicharge from the pipe i 6.50 x -3 m 3 /. A) Find the
More informationThe Dominant Thermal Resistance Approach for Heat Transfer to Supercritical-Pressure Fluids
The Dominant Thermal Resistance Approach for Heat Transfer to Supercritical-Pressure Fluids Donald M. McEligot 1,2, Eckart Laurien 3, Shuisheng He 4 and Wei Wang 4,5 1. Nuclear Engineering Division, U.
More informationEvapotranspiration: Theory and Applications
Evapotranspiration: Theory and Applications Lu Zhang ( 张橹 ) CSIRO Land and Water Evaporation: part of our everyday life Evapotranspiration Global Land: P = 800 mm Q = 315 mm E = 485 mm Evapotranspiration
More informationThe Meaning and Significance of Heat Transfer Coefficient. Alan Mueller, Chief Technology Officer
The Meaning and Significance of Heat Transfer Coefficient Alan Mueller, Chief Technology Officer The Meaning of Heat Transfer Coefficient I kno the meaning of HTC! Why should I aste my time listening to
More informationLand Surface Processes and Their Impact in Weather Forecasting
Land Surface Processes and Their Impact in Weather Forecasting Andrea Hahmann NCAR/RAL with thanks to P. Dirmeyer (COLA) and R. Koster (NASA/GSFC) Forecasters Conference Summer 2005 Andrea Hahmann ATEC
More informationCHAPTER 8 ENTROPY. Blank
CHAPER 8 ENROPY Blank SONNAG/BORGNAKKE SUDY PROBLEM 8-8. A heat engine efficiency from the inequality of Clausius Consider an actual heat engine with efficiency of η working between reservoirs at and L.
More informationEng Thermodynamics I conservation of mass; 2. conservation of energy (1st Law of Thermodynamics); and 3. the 2nd Law of Thermodynamics.
Eng3901 - Thermodynamics I 1 1 Introduction 1.1 Thermodynamics Thermodynamics is the study of the relationships between heat transfer, work interactions, kinetic and potential energies, and the properties
More informationThermodynamics ENGR360-MEP112 LECTURE 7
Thermodynamics ENGR360-MEP11 LECTURE 7 Thermodynamics ENGR360/MEP11 Objectives: 1. Conservation of mass principle.. Conservation of energy principle applied to control volumes (first law of thermodynamics).
More informationIntroduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles
Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles by James Doane, PhD, PE Contents 1.0 Course Oeriew... 4.0 Basic Concepts of Thermodynamics... 4.1 Temperature
More informationMAE 101A. Homework 3 Solutions 2/5/2018
MAE 101A Homework 3 Solution /5/018 Munon 3.6: What preure gradient along the treamline, /d, i required to accelerate water upward in a vertical pipe at a rate of 30 ft/? What i the anwer if the flow i
More informationdf dz = dp dt Essentially, this is just a statement of the first law in one of the forms we derived earlier (expressed here in W m 3 ) dq p dt dp
A problem with using entropy as a variable is that it is not a particularly intuitive concept. The mechanics of using entropy for evaluating system evolution is well developed, but it sometimes feels a
More informationKelvin Effect. Covers Reading Material in Chapter 10.3 Atmospheric Sciences 5200 Physical Meteorology III: Cloud Physics
Kelvin Effect Covers Reading Material in Chapter 10.3 Atmospheric Sciences 5200 Physical Meteorology III: Cloud Physics Vapor Pressure (e) e < e # e = e # Vapor Pressure e > e # Relative humidity RH =
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 informationSupersonic Flow Turning
Supersonic Flow Turning For normal shocks, flow is perpendicular to shock no change in flow direction How does supersonic flow change direction, i.e., make a turn either slow to subsonic ahead of turn
More informationExternal Flow: Flow over Bluff Objects (Cylinders, Spheres, Packed Beds) and Impinging Jets
External Flow: Flow over Bluff Object (Cylinder, Sphere, Packed Bed) and Impinging Jet he Cylinder in Cro Flow - Condition depend on pecial feature of boundary layer development, including onet at a tagnation
More informationFLUID MECHANICS EQUATIONS
FLUID MECHANIC EQUATION M. Ragheb 11/2/2017 INTRODUCTION The early part of the 18 th -century saw the burgeoning of the field of theoretical fluid mechanics pioneered by Leonhard Euler and the father and
More informationLecture notes: Interception and evapotranspiration
Lecture notes: Interception and evapotranspiration I. Vegetation canopy interception (I c ): Portion of incident precipitation (P) physically intercepted, stored and ultimately evaporated from vegetation
More informationV (r,t) = i ˆ u( x, y,z,t) + ˆ j v( x, y,z,t) + k ˆ w( x, y, z,t)
IV. DIFFERENTIAL RELATIONS FOR A FLUID PARTICLE This chapter presents the development and application of the basic differential equations of fluid motion. Simplifications in the general equations and common
More informationToday s Lecture: Atmosphere finish primitive equations, mostly thermodynamics
Today s Lecture: Atmosphere finish primitive equations, mostly thermodynamics Reference Peixoto and Oort, Sec. 3.1, 3.2, 3.4, 3.5 (but skip the discussion of oceans until next week); Ch. 10 Thermodynamic
More informationLecture 3a: Surface Energy Balance
Lecture 3a: Surface Energy Balance Instructor: Prof. Johnny Luo http://www.sci.ccny.cuny.edu/~luo Total: 50 pts Absorption of IR radiation O 3 band ~ 9.6 µm Vibration-rotation interaction of CO 2 ~
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 informationSection 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow
Section 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow Anderson: Chapter 2 pp. 41-54 1 Equation of State: Section 1 Review p = R g T " > R g = R u M w - R u = 8314.4126
More informationLecture 3a: Surface Energy Balance
Lecture 3a: Surface Energy Balance Instructor: Prof. Johnny Luo http://www.sci.ccny.cuny.edu/~luo Surface Energy Balance 1. Factors affecting surface energy balance 2. Surface heat storage 3. Surface
More informationHalliday/Resnick/Walker 7e Chapter 14
HRW 7e Chapter 4 Page of 8 Halliday/Resnick/Walker 7e Chapter 4. The air inside pushes outard ith a force given by p i A, here p i is the pressure inside the room and A is the area of the indo. Similarly,
More informationIF YOU CAN T SOLVE PROBLEM 1, ASSUME stability = D, width = 400m, height = 400m, flow = 10 6 m 3 /s
NAME: 75 MINUTES; HAND IN YOUR 1 SHEET OF NOTES WITH THE EXAM; ASK FOR EXTRA PAPER IF NEEDED. MAKE (AND STATE) ANY REASONABLE ASSUMPTIONS NECESSARY TO GET AN ANSWER IN ADDITION TO THOSE GIVEN. CHECKING
More informationDiffusional Growth of Liquid Phase Hydrometeros.
Diffusional Growth of Liquid Phase Hydrometeros. I. Diffusional Growth of Liquid Phase Hydrometeors A. Basic concepts of diffusional growth. 1. To understand the diffusional growth of a droplet, we must
More informationChapter 6. Using Entropy
Chapter 6 Using Entropy Learning Outcomes Demonstrate understanding of key concepts related to entropy and the second law... including entropy transfer, entropy production, and the increase in entropy
More informationEric. W. Harmsen 1, John Mecikalski 2, Pedro Tosado Cruz 1 Ariel Mercado Vargas 1
Estimating Evapotranspiration using Satellite Remote Sensing in Puerto Rico, Haiti and the Dominican Republic Eric. W. Harmsen 1, John Mecikalski 2, Pedro Tosado Cruz 1 Ariel Mercado Vargas 1 1. University
More informationLesson 6 Review of fundamentals: Fluid flow
Lesson 6 Review of fundamentals: Fluid flow The specific objective of this lesson is to conduct a brief review of the fundamentals of fluid flow and present: A general equation for conservation of mass
More informationChapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky
Chapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky School of Chemical, Biological, and Enironmental Engineering Oregon State Uniersity 1.1 (b) The olume of water
More informationChapter 5. Mass and Energy Analysis of Control Volumes
Chapter 5 Mass and Energy Analysis of Control Volumes Conservation Principles for Control volumes The conservation of mass and the conservation of energy principles for open systems (or control volumes)
More informationCHAPTER 4 The Integral Forms of the Fundamental Laws
CHAPTER 4 The Integral Forms of the Fundamental Laws FE-type Exam Review Problems: Problems 4- to 4-5 4 (B) 4 (D) 4 (A) 44 (D) p m ρa A π 4 7 87 kg/s RT 87 9 Refer to the circle of Problem 47: 757 Q A
More information1. Intensity of Periodic Sound Waves 2. The Doppler Effect
1. Intenity o Periodic Sound Wae. The Doppler Eect 1-4-018 1 Objectie: The tudent will be able to Deine the intenity o the ound wae. Deine the Doppler Eect. Undertand ome application on ound 1-4-018 3.3
More informationSnow Melt with the Land Climate Boundary Condition
Snow Melt with the Land Climate Boundary Condition GEO-SLOPE International Ltd. www.geo-slope.com 1200, 700-6th Ave SW, Calgary, AB, Canada T2P 0T8 Main: +1 403 269 2002 Fax: +1 888 463 2239 Introduction
More informationGoogle Earth Engine METRIC (GEM) Application for Remote Sensing of Evapotranspiration
Google Earth Engine METRIC (GEM) Application for Remote Sensing of Evapotranspiration Nadya Alexander Sanchez, Quinn Hart, Justin Merz, and Nick Santos Center for Watershed Sciences University of California,
More informationPhysical Fundamentals of Global Change Processes
University of Applied Sciences Eberswalde Master Study Program Global Change Management Manfred Stock Potsdam Institute for Climate Impact Research Module: Physical Fundamentals of Global Change Processes
More informationATMO 551a Moist Adiabat Fall Change in internal energy: ΔU
Enthalpy and the Moist Adiabat We have described the dry adiabat where an air parcel is lifted rapidly causing the air parcel to expand as the environmental pressure decreases and the air parcel does work
More information( ) Given: In a constant pressure combustor. C4H10 and theoretical air burns at P1 = 0.2 MPa, T1 = 600K. Products exit at P2 = 0.
(SP 9) N-butane (C4H1) i burned with 85 percent theoretical air, and the product of combution, an equilibrium mixture containing only O, CO, CO, H, HO, N, and NO, exit from a combution chamber at K,. MPa.
More information2b m 1b: Sat liq C, h = kj/kg tot 3a: 1 MPa, s = s 3 -> h 3a = kj/kg, T 3b
.6 A upercritical team power plant ha a high preure of 0 Ma and an exit condener temperature of 50 C. he maximum temperature in the boiler i 000 C and the turbine exhaut i aturated vapor here i one open
More informationEstimating Evaporation : Principles, Assumptions and Myths. Raoul J. Granger, NWRI
Estimating Evaporation : Principles, Assumptions and Myths Raoul J. Granger, NWRI Evaporation So what is it anyways? Evaporation is the phenomenon by which a substance is converted from the liquid or solid
More informationRadiative equilibrium Some thermodynamics review Radiative-convective equilibrium. Goal: Develop a 1D description of the [tropical] atmosphere
Radiative equilibrium Some thermodynamics review Radiative-convective equilibrium Goal: Develop a 1D description of the [tropical] atmosphere Vertical temperature profile Total atmospheric mass: ~5.15x10
More informationChapter 5: The First Law of Thermodynamics: Closed Systems
Chapter 5: The First Law of Thermodynamics: Closed Systems The first law of thermodynamics can be simply stated as follows: during an interaction between a system and its surroundings, the amount of energy
More informationME 3560 Fluid Mechanics
Sring 018 ME 3560 Fluid Mechanic Chater III. Elementary Fluid Dynamic The Bernoulli Equation 1 Sring 018 3.1 Newton Second Law A fluid article can exerience acceleration or deceleration a it move from
More informationThermodynamics 1. Lecture 7: Heat transfer Open systems. Bendiks Jan Boersma Thijs Vlugt Theo Woudstra. March 1, 2010.
hermodynamics Lecture 7: Heat transfer Open systems Bendiks Jan Boersma hijs Vlugt heo Woudstra March, 00 Energy echnology Summary lecture 6 Poisson relation efficiency of a two-stroke IC engine (Otto
More informationT098. c Dr. Md. Zahurul Haq (BUET) First Law of Thermodynamics ME 201 (2012) 2 / 26
Conservation of Energy for a Closed System Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-, Bangladesh zahurul@me.buet.ac.bd
More informationConsequences of Second Law of Thermodynamics. Entropy. Clausius Inequity
onsequences of Second Law of hermodynamics Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & echnology BUE Dhaka-000, Bangladesh zahurul@me.buet.ac.bd
More informationMAE 320 THERODYNAMICS FINAL EXAM - Practice. Name: You are allowed three sheets of notes.
50 MAE 320 THERODYNAMICS FINAL EXAM - Practice Name: You are allowed three sheets of notes. 1. Fill in the blanks for each of the two (Carnot) cycles below. (a) 5 a) Heat engine or Heat pump/refrigerator
More information2.25 Advanced Fluid Mechanics
MIT Department of Mechanical Engineering.5 Advanced Fluid Mechanics Problem 4.05 This problem is from Advanced Fluid Mechanics Problems by A.H. Shapiro and A.A. Sonin Consider the frictionless, steady
More informationChapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 5 Mass and Energy Analysis of Control Volumes by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics:
More informationTypes of Heat Transfer
ype of Heat ranfer * Dvz Dt x k d dx v S * * v Gr z HH vap lat uject in the coure conduction (Fourier Law) forced convection (due to flow) ource term free convection (fluid motion due to denity variation
More informationContents. 1. Evaporation
Contents 1 Evaporation 1 1a Evaporation from Wet Surfaces................... 1 1b Evaporation from Wet Surfaces in the absence of Advection... 4 1c Bowen Ratio Method........................ 4 1d Potential
More informationMICRO-HYDRO INSTALLATION SIZING CALCULATIONS Jacques Chaurette eng. January 17, 2008
MICRO-HYDRO INSTALLATION SIZING CALCULATIONS Jacque Chaurette eng. January 7, 008 Calculation for micro-hydro ine jet impact elocity are baed on the ame ort of calculation done for pump ytem, except there
More informationELECTROMAGNETIC WAVES AND PHOTONS
CHAPTER ELECTROMAGNETIC WAVES AND PHOTONS Problem.1 Find the magnitude and direction of the induced electric field of Example.1 at r = 5.00 cm if the magnetic field change at a contant rate from 0.500
More informationIntroduction CHAPTER Prime Movers. 1.2 Sources of Energy
Introduction CHAPTER 1 1.1 Prime Movers Prime mover is a device which converts natural source of energy into mechanical work to drive machines for various applications. In olden days, man had to depend
More informationChapter 5: Mass, Bernoulli, and
and Energy Equations 5-1 Introduction 5-2 Conservation of Mass 5-3 Mechanical Energy 5-4 General Energy Equation 5-5 Energy Analysis of Steady Flows 5-6 The Bernoulli Equation 5-1 Introduction This chapter
More informationPh.D. Qualifying Exam in Fluid Mechanics
Student ID Department of Mechanical Engineering Michigan State University East Lansing, Michigan Ph.D. Qualifying Exam in Fluid Mechanics Closed book and Notes, Some basic equations are provided on an
More informationEvapotranspiration. Here, liquid water on surfaces or in the very thin surface layer of the soil that evaporates directly to the atmosphere
Evapotranspiration Evaporation (E): In general, the change of state from liquid to gas Here, liquid water on surfaces or in the very thin surface layer of the soil that evaporates directly to the atmosphere
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 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 informationChapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
5- Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL OLUMES Conseration of Mass 5-C Mass, energy, momentum, and electric charge are consered, and olume and entropy are not consered durg a process. 5-C Mass
More informationNon-Newtonian fluids is the fluids in which shear stress is not directly proportional to deformation rate, such as toothpaste,
CHAPTER1: Basic Definitions, Zeroth, First, and Second Laws of Thermodynamics 1.1. Definitions What does thermodynamic mean? It is a Greeks word which means a motion of the heat. Water is a liquid substance
More informationFundamental Concepts of Convection : Flow and Thermal Considerations. Chapter Six and Appendix D Sections 6.1 through 6.8 and D.1 through D.
Fundamental Concepts of Convection : Flow and Thermal Considerations Chapter Six and Appendix D Sections 6.1 through 6.8 and D.1 through D.3 6.1 Boundary Layers: Physical Features Velocity Boundary Layer
More informationChapter 4 Water Vapor
Chapter 4 Water Vapor Chapter overview: Phases of water Vapor pressure at saturation Moisture variables o Mixing ratio, specific humidity, relative humidity, dew point temperature o Absolute vs. relative
More informationME 331 Homework Assignment #6
ME 33 Homework Assignment #6 Problem Statement: ater at 30 o C flows through a long.85 cm diameter tube at a mass flow rate of 0.020 kg/s. Find: The mean velocity (u m ), maximum velocity (u MAX ), and
More informationAnalysis of cylindrical heat pipes incorporating the e ects of liquid±vapor coupling and non-darcian transportða closed form solution
International Journal of Heat and Mass Transfer 42 (1999) 3405±341 Analysis of cylindrical heat pipes incorporating the e ects of liquid±apor coupling and non-darcian transportða closed form solution N.
More informationE d. h, c o, k are all parameters from quantum physics. We need not worry about their precise definition here.
The actual form of Plank s law is: b db d b 5 e C C2 1 T 1 where: C 1 = 2hc o 2 = 3.7210 8 Wm /m 2 C 2 = hc o /k = 1.3910 mk Where: h, c o, k are all parameters from quantum physics. We need not worry
More informationDynamic Van der Waals Theory
Dynamic Van der Waal heory A diffue interface model for two-phae hydrodynamic involving the liquid-ga tranition in non-uniform temperature [A. Onuki, PRL (005) & PRE (007)] Hydrodynamic equation for liquid-ga
More informationAtmospheric Sciences 321. Science of Climate. Lecture 13: Surface Energy Balance Chapter 4
Atmospheric Sciences 321 Science of Climate Lecture 13: Surface Energy Balance Chapter 4 Community Business Check the assignments HW #4 due Wednesday Quiz #2 Wednesday Mid Term is Wednesday May 6 Practice
More informationME 201 Thermodynamics
Spring 01 ME 01 Thermodynamics Property Evaluation Practice Problems II Solutions 1. Air at 100 K and 1 MPa goes to MPa isenthapically. Determine the entropy change. Substance Type: Ideal Gas (air) Process:
More informationA Model Answer for. Problem Set #4 FLUID DYNAMICS
A Model Answer for Problem Set #4 FLUID DYNAMICS Problem. Some elocity measurements in a threedimensional incomressible flow field indicate that u = 6xy and = -4y z. There is some conflicting data for
More informationPlanetary Atmospheres
Planetary Atmospheres Structure Composition Meteorology Clouds Photochemistry Atmospheric Escape EAS 4803/8803 - CP 20:1 Cloud formation Saturated Vapor Pressure: Maximum amount of water vapor partial
More information