kg m kg kg m =1 slope

Size: px
Start display at page:

Download "kg m kg kg m =1 slope"

Transcription

1 (5) Win loa Wen structure blocks te flow of win, te win's kinetic energy is converte into otential energy of ressure, wic causes a win loaing. ensity an velocity of air te angle of incience of te win 3 te sae an stiffness of te structure 4 te rougness of its surface Analysis: static or ynamic () For static aroac, mean win ressure can be aroximate: V q=, ρ= te ensity of air, V= te win velocity (kinetic energy) kg m kg kg m unit : ressure( N / m ) 3 m sec m.sec m sec - Groun elevation is imortant te velocity of te win increases wit elevation. Te iger te structure, te more severe win loaing becomes. - Once te mean ressure q as been calculate, its magnitue is multilie by various coefficients to obtain esign static ressure tat is alie to te structure. Imortance of te structure Possibility of win gust 3 Te ressure ifference outsie an insie te structure () Dynamic aroac for ig rise builing Win tunnel tests - fining te ressure effects on te builing Static Aroac ASE 7-0 stanar q= V is moifie to account for te imortance of te structure, its eigt, an terrain. (win ressure) q K K K V 0.63 (N/m²) K : velocity ressure exosure coefficient eigt, terrain (0.85~.09) Table.5 K : a factor tat accounts for win see increase ue to ills an escarments. For flat groun level K = sloe K : a factor accounting for te irection of te win. (Only nee subjecte to te combinations of loas). For win acting alone, K = V : velocity in m/sec of a 3 secon gust of win measure at 0m above te groun tat as a 50 year recurrence erio. From a win ma (47 m/sec for agricultural an storage builings, 54m/sec for osital) DESIGN WIND PRESSURE Once te value of q ( q 0.63 K K K V can be etermine from a list of relevant equations liste in ASE 7-0 stanars. ) is obtaine, te esign ressure Te coice te flexibility eigt of te structure 3weter te esign for te main win-force resisting system, or for te builing s comonents an claing. For examle, for a conservative esign win ressure on nonflexible builings of any eigt is etermine using qg q ( G ) (N/m²) i q = q for winwar wall at eigt above te groun q = q for leewar wall, sie walls, an roof were = (: mean eigt of roof)

2 G: a win guest effect factor Exosure. For a rigi structure, G=0.85 : wall or roof ressure coefficient etermine from ( Table (a):wall Table (b):roof G : internal ressure coefficient tyes of oening in te builing. i For fully enclose builings ( G i ) = ±0.8 in Fig -3) EX -3 Given V = 47 m/s (See of 3secon gust win measure at 0m above groun level for 50 year recurrence erio) K = for flat terrain K = only win loaing is consiere win ressure q 0.63K K K V = 0.63* K ***47²=354* K eigt () calculate q (: mean eigt of te roof) [use for leewar later] = tan 0 / = /= 9.48m For, linear interolation for = using able K ( 9.) 0.98 at = (mean eigt). 9. At = 9.48, K Z =K Z= = K =0.987 q q = 354 K = 354x0.997=337 N/m² 3 esign win ressure = qg - q ( G ) i = q(0.85) -337( 0.8) = 0.85q 4 from Table -5 an K ( 9.) (m) K q (N/m ) G = 0.85(gust factor) G = ±0.8 for fully enclose builing i q = 354 K =

3 () Winwar wall for all L/B, = 0.8 (winwar) q=q =0.85q q = or = = 54 N/m² =04 N/m² 6. = = 588 N/m² or 070 N/m² 7.6 =65 N/m² or 07 N/m² ()q= q Leewar wall for L/B = (.5)/45 =, = -0.5 = 0.85 q q + 4 = (-0.5) -4 = -809 N/m² or -37 N/m² (3)q= q sie wall for all L/B = = 0.85 q -4=-037 N/m² or -555 N/m² (4)q= q winwar roof for /L=9.48/(x.5) = 0. < 0.5 =-0.7 = 0.85 q -4= -037 N/m² or -555 N/m² (5)q= q Leewar wall roof =-0.3 = -58 N/m² or -00 N/m² +ressure - suction Te frame structure must resist tese loaings as well as loaings calculate from win blowing on te front or rear of te builing. Design win ressure for signs. F=q G f A s Here, q = te win ressure at te eigt, measure from te groun to te to of te sign G = te win-gust coefficient factor f = a force coefficient wic eens uon te asect ratio (wit B of te sign to te eigt s of te sign), an te clear area ratio (sign eigt s to te elevation, measure from te groun to te to of te sign). A s = te area of te face of te sign rojecte into te win in m TABLE -6 (B/s=4) Force oefficients for Above-Groun Soli Signs, f s/ f

4 (6) Snow & Ice loa ANSI ASE 7-0 Snow / ice treate as static roof loas. Base on a groun snow converte to roof conversion. Use 50 years recurrence interval Geograical mas For flat roof (sloe <5%) P f (kn/m ) = 0.7 e t I s g Here, e exosure factor eening on terrain (0.8: exose roof in an unobstructe area,.: oterwise) t = imensionless termal factor (.: for uneate structure,.0: for eate structure) I s = imortance factor (0.8 for agriculture builings,. for scools an ositals) g = groun snow loa if g 0.96 kn/m P f = max(i g, 0.7 e t I s g ) if g > 0.96 kn/m P f = Iⅹ0.96 kn/m For sloe roof P s = s P f Here, s = sloe factor (0~.0) sloe & termal factors [EXAMPLE -4] Te uneate storage facility sown in Fig -5 is locate on flat oen terrain in central Illinois, were te groun snow loa is 0.7 kn/m. Determine te esign snow loa on te roof (4% sloe). <Solution> Given groun snow loa = 0.7 kn/m, oen terrain e = 0.8, uneate storage t =., I = 0.8 Since g = kn/m, P f = max(i g, 0.7 e t I s g ) P f = 0.7 e t I s g = 0.7ⅹ0.8ⅹ.ⅹ0.8ⅹ0.7 = 0.39 kn/m P f = I g =0.8ⅹ0.7 = 0.58 kn/m P f = max(0.58, 0.39) = 0.58 kn/m (7) Eartquake loas During an Eartquake te groun vibrates bot oriontally an vertically. Te vertical motion is sligt an is usually neglecte in esign. - Eartquake rouce loaings troug its interaction wit te groun & its resonse caracteristics - Teir magnitue eens on amount & tye of groun acceleration, mass & stiffness of structure - To block is te lume mass of te roof - Mile block is te lume stiffness of all te builing s columns - During eartquake, te groun vibrates bot oriontally & vertically S S DS R / I R: resonse moification factor I: imortance factor S : sectral resonse acceleration DS (8) Hyrostatic an Soil ressure Wen a structure is nee to retain water, soil, or granular materials, ressures eveloe by loaings become an imortant criterion for teir esign. (retaining walls) 4

5 (9) Oter natural loas Effect of blast, temerature canges, ifferential settlement. Structural Design Material uncertainties occur ue to - variability in material roerties - resiual stress in materials - intene measurements being ifferent from fabricate sies - material corrosion or ecay Many tyes of loas can occur simultaneously on a structure Allowable stress esign (or working stress esign): comute elastic stress in material must not excee te allowable stress along wit te following tyical loa combinations: (D: ea loa, L: live loa, S: snow loa, L r : roof live loa, W: win loa, E: eartquake loa) D D L 3 D Lr or S or R 4 D 0.75 L 0.75 Lr or S or R 5 D W or 0.7E 6 D 0.75 W or 0.7 E 0.75 L 0.75 Lr or S or R 70.6 D W or 0.7E Strengt Design (or Loa Resistance Factor Design, LRFD): te eman from ultimate loa calculate by te following loa combinations must not excee ultimate strengt of critical sections. In strengt esign, material uncertainty an loa uncertainty are searately etermine. ().4D (). D.6 L 0.5 Lr or S or R (3). D.6 L or S or R 0.5 L or 0.8W r (4). D.6 W 0.5 L 0.5 Lr or S or R (5). D.0 E 0.5 L 0.S (6)0.9 D.6 W or.0e Plastic esign: eveloe for steel frames 5

The thermal wind 1. v g

The thermal wind 1. v g The thermal win The thermal win Introuction The geostrohic win is etermine by the graient of the isobars (on a horizontal surface) or isohyses (on a ressure surface). On a ressure surface the graient of

More information

Example 1. Examples for walls are available on our Web page: Columns

Example 1. Examples for walls are available on our Web page:   Columns Portlan Cement Association Page 1 o 9 Te ollowing examples illustrate te esign metos presente in te article Timesaving Design Ais or Reinorce Concrete, Part 3: an Walls, by Davi A. Fanella, wic appeare

More information

0.1 Differentiation Rules

0.1 Differentiation Rules 0.1 Differentiation Rules From our previous work we ve seen tat it can be quite a task to calculate te erivative of an arbitrary function. Just working wit a secon-orer polynomial tings get pretty complicate

More information

On my honor, I have neither given nor received unauthorized aid on this examination.

On my honor, I have neither given nor received unauthorized aid on this examination. Instructor(s): iel/uric PHYSICS DEPARTENT PHY 2053 Exam 1 October 3, 2012 Name (print, last first): Signature: On my onor, I ave neiter given nor receive unautorize ai on tis examination. YOUR TEST NUBER

More information

Phy 231 Sp 02 Homework #6 Page 1 of 4

Phy 231 Sp 02 Homework #6 Page 1 of 4 Py 231 Sp 02 Homework #6 Page 1 of 4 6-1A. Te force sown in te force-time diagram at te rigt versus time acts on a 2 kg mass. Wat is te impulse of te force on te mass from 0 to 5 sec? (a) 9 N-s (b) 6 N-s

More information

Lecture Notes Di erentiating Trigonometric Functions page 1

Lecture Notes Di erentiating Trigonometric Functions page 1 Lecture Notes Di erentiating Trigonometric Functions age (sin ) 7 sin () sin 8 cos 3 (tan ) sec tan + 9 tan + 4 (cot ) csc cot 0 cot + 5 sin (sec ) cos sec tan sec jj 6 (csc ) sin csc cot csc jj c Hiegkuti,

More information

1 Lecture 13: The derivative as a function.

1 Lecture 13: The derivative as a function. 1 Lecture 13: Te erivative as a function. 1.1 Outline Definition of te erivative as a function. efinitions of ifferentiability. Power rule, erivative te exponential function Derivative of a sum an a multiple

More information

Analysis: The speed of the proton is much less than light speed, so we can use the

Analysis: The speed of the proton is much less than light speed, so we can use the Section 1.3: Wave Proerties of Classical Particles Tutorial 1 Practice, age 634 1. Given: 1.8! 10 "5 kg # m/s; 6.63! 10 "34 J #s Analysis: Use te de Broglie relation, λ. Solution:! 6.63 " 10#34 kg $ m

More information

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine?

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine? 1 1 Power is transferred troug a macine as sown. power input P I macine power output P O power loss P L Wat is te efficiency of te macine? P I P L P P P O + P L I O P L P O P I 2 ir in a bicycle pump is

More information

This section outlines the methodology used to calculate the wave load and wave wind load values.

This section outlines the methodology used to calculate the wave load and wave wind load values. COMPUTERS AND STRUCTURES, INC., JUNE 2014 AUTOMATIC WAVE LOADS TECHNICAL NOTE CALCULATION O WAVE LOAD VALUES This section outlines the methoology use to calculate the wave loa an wave win loa values. Overview

More information

10 CV 35 FLUID MECHANICS NOTES UNIT-2 PRESSURE AND ITS MEASUREMENT. Dr. Nagaraj Sitaram, Professor, Civil Department, SBMJCE, Bangalore

10 CV 35 FLUID MECHANICS NOTES UNIT-2 PRESSURE AND ITS MEASUREMENT. Dr. Nagaraj Sitaram, Professor, Civil Department, SBMJCE, Bangalore 10 CV 35 FLUID MECHNICS NOTES UNIT-2 PRESSURE ND ITS MESUREMENT by UNIT-2 PRESSURE ND ITS MESUREMENT 2.0 INTRODUCTION: Fluid is a state of matter wic exibits te roerty of flow. Wen a certain mass of fluids

More information

Mechanical Vibrations Misc Topics Base Excitation & Seismic

Mechanical Vibrations Misc Topics Base Excitation & Seismic Mechanical Vibrations Misc Topics Base Excitation & Seismic Peter Avitabile Mechanical Engineering Department University of Massachusetts Lowell 1 Dr. Peter Avitabile Seismic events are often moele with

More information

SEISMIC PASSIVE EARTH PRESSURE WITH VARYING SHEAR MODULUS: PSEUDO-DYNAMIC APPROACH

SEISMIC PASSIVE EARTH PRESSURE WITH VARYING SHEAR MODULUS: PSEUDO-DYNAMIC APPROACH IGC 29, Guntur, INDIA SEISMIC PASSIE EART PRESSURE WIT ARYING SEAR MODULUS: PSEUDO-DYNAMIC APPROAC P. Gos Assistant Professor, Deartment of Ciil Engineering, Indian Institute of Tecnology Kanur, Kanur

More information

ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA

ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA International Journal of Moern Physics B Vol. 24, Nos. 15 & 16 (21) 347 352 Worl Scientific Publishing Comany DOI: 1.1142/S217979216669 ANALYSIS OF PNEUMATIC FINE PARTICLE PEENING PROCESS BY USING A HIGH-SPEED-CAMERA

More information

Polarizability of a metallic nanosphere: Local random-phase approximation (LRPA)

Polarizability of a metallic nanosphere: Local random-phase approximation (LRPA) Sri Lankan Journal of Pysics, Vol. 1(1) (01) 41-47 Institute of Pysics - Sri Lanka Researc Article Polarizability of a metallic nanosere: Local random-ase aroximation (LRPA) Prabat Hewageegana * Deartment

More information

Solutions to Homework #05 MATH ln z 2 + x 2 1 = 2x2 z 2 + x 2 + ln z2 + x 2. = x. ln z 2 + x 2 2z z 2 + x 2 = 2xz

Solutions to Homework #05 MATH ln z 2 + x 2 1 = 2x2 z 2 + x 2 + ln z2 + x 2. = x. ln z 2 + x 2 2z z 2 + x 2 = 2xz Solutions to Homeork #05 MATH Kaai Section. (I) Exercise #. g x and g z : Product Rule: g x = x @ ln z + x + ln z + x @ [x] = x x z + x + ln z + x = x z + x + ln z + x x is eld constant. g z = x @ ln z

More information

CHS GUSSET PLATE CONNECTIONS ANALYSES Theoretical and Experimental Approaches

CHS GUSSET PLATE CONNECTIONS ANALYSES Theoretical and Experimental Approaches EUROSTEEL 8, 3-5 Setember 8, Graz, Austria 561 CHS GUSSET PLATE CONNECTIONS ANALYSES Theoretical an Exerimental Aroaches Arlene M. S. Freitas a, Daniela G. V. Minchillo b, João A. V. Requena c, Afonso

More information

106 PHYS - CH6 - Part2

106 PHYS - CH6 - Part2 106 PHYS - CH6 - Part Conservative Forces (a) A force is conservative if work one by tat force acting on a particle moving between points is inepenent of te pat te particle takes between te two points

More information

Derivatives. if such a limit exists. In this case when such a limit exists, we say that the function f is differentiable.

Derivatives. if such a limit exists. In this case when such a limit exists, we say that the function f is differentiable. Derivatives 3. Derivatives Definition 3. Let f be a function an a < b be numbers. Te average rate of cange of f from a to b is f(b) f(a). b a Remark 3. Te average rate of cange of a function f from a to

More information

Non-linear Analysis Method of Ground Response Using Equivalent Single-degree-of-freedom Model

Non-linear Analysis Method of Ground Response Using Equivalent Single-degree-of-freedom Model Proceedings of te Tent Pacific Conference on Eartquake Engineering Building an Eartquake-Resilient Pacific 6-8 November 25, Sydney, Australia Non-linear Analysis Metod of Ground Response Using Equivalent

More information

Discharge initiation and plasma column formation in aspect ratio A=2 tokamak.

Discharge initiation and plasma column formation in aspect ratio A=2 tokamak. Discharge initiation an lasma column formation in asect ratio A toama... Khayrutinov E.A. Azizov, A.D. Baralov, G.G.Glaush, I.L.Taibaeva, Ph.W.West 3 Troits, Moscow eg., ussia NNC, K 3 General Atomics,

More information

Chapter Primer on Differentiation

Chapter Primer on Differentiation Capter 0.01 Primer on Differentiation After reaing tis capter, you soul be able to: 1. unerstan te basics of ifferentiation,. relate te slopes of te secant line an tangent line to te erivative of a function,.

More information

Reminder: Exam 3 Friday, July 6. The Compton Effect. General Physics (PHY 2140) Lecture questions. Show your work for credit.

Reminder: Exam 3 Friday, July 6. The Compton Effect. General Physics (PHY 2140) Lecture questions. Show your work for credit. General Pysics (PHY 2140) Lecture 15 Modern Pysics Cater 27 1. Quantum Pysics Te Comton Effect Potons and EM Waves Wave Proerties of Particles Wave Functions Te Uncertainty Princile Reminder: Exam 3 Friday,

More information

In Leibniz notation, we write this rule as follows. DERIVATIVE OF A CONSTANT FUNCTION. For n 4 we find the derivative of f x x 4 as follows: lim

In Leibniz notation, we write this rule as follows. DERIVATIVE OF A CONSTANT FUNCTION. For n 4 we find the derivative of f x x 4 as follows: lim .1 DERIVATIVES OF POLYNOIALS AND EXPONENTIAL FUNCTIONS c =c slope=0 0 FIGURE 1 Te grap of ƒ=c is te line =c, so fª()=0. In tis section we learn ow to ifferentiate constant functions, power functions, polnomials,

More information

Chapter A 9.0-V battery is connected to a lightbulb, as shown below. 9.0-V Battery. a. How much power is delivered to the lightbulb?

Chapter A 9.0-V battery is connected to a lightbulb, as shown below. 9.0-V Battery. a. How much power is delivered to the lightbulb? Capter continued carges on te plates were reversed, te droplet would accelerate downward since all forces ten act in te same direction as gravity. 5. A 0.5-F capacitor is able to store 7.0 0 C of carge

More information

160 Chapter 3: Differentiation

160 Chapter 3: Differentiation 3. Differentiation Rules 159 3. Differentiation Rules Tis section introuces a few rules tat allow us to ifferentiate a great variety of functions. By proving tese rules ere, we can ifferentiate functions

More information

This file is /conf/snippets/setheader.pg you can use it as a model for creating files which introduce each problem set.

This file is /conf/snippets/setheader.pg you can use it as a model for creating files which introduce each problem set. Yanimov Almog WeBWorK assignment number Sections 3. 3.2 is ue : 08/3/207 at 03:2pm CDT. Te (* replace wit url for te course ome page *) for te course contains te syllabus, graing policy an oter information.

More information

does NOT exist. WHAT IF THE NUMBER X APPROACHES CANNOT BE PLUGGED INTO F(X)??????

does NOT exist. WHAT IF THE NUMBER X APPROACHES CANNOT BE PLUGGED INTO F(X)?????? MATH 000 Miterm Review.3 Te it of a function f ( ) L Tis means tat in a given function, f(), as APPROACHES c, a constant, it will equal te value L. Tis is c only true if f( ) f( ) L. Tat means if te verticle

More information

FE FORMULATIONS FOR PLASTICITY

FE FORMULATIONS FOR PLASTICITY G These slides are designed based on the book: Finite Elements in Plasticity Theory and Practice, D.R.J. Owen and E. Hinton, 1970, Pineridge Press Ltd., Swansea, UK. 1 Course Content: A INTRODUCTION AND

More information

Rules of Differentiation

Rules of Differentiation LECTURE 2 Rules of Differentiation At te en of Capter 2, we finally arrive at te following efinition of te erivative of a function f f x + f x x := x 0 oing so only after an extene iscussion as wat te

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY O SASKATCHEWAN Department of Pysics and Engineering Pysics Pysics 117.3 MIDTERM EXAM Regular Sitting NAME: (Last) Please Print (Given) Time: 90 minutes STUDENT NO.: LECTURE SECTION (please ceck):

More information

The OPS-model. Ferd Sauter Margreet van Zanten Eric van der Swaluw Jan Aben Frank de Leeuw Hans van Jaarsveld. Description of OPS 4.5.

The OPS-model. Ferd Sauter Margreet van Zanten Eric van der Swaluw Jan Aben Frank de Leeuw Hans van Jaarsveld. Description of OPS 4.5. Te OPS-model Descrition of OPS 4.5. Ferd Sauter Margreet van Zanten Eric van der Swaluw Jan Aben Frank de Leeuw Hans van Jaarsveld National Institute for Public Healt and te Environment RIVM os_v4_5 834.doc,

More information

Chapters 19 & 20 Heat and the First Law of Thermodynamics

Chapters 19 & 20 Heat and the First Law of Thermodynamics Capters 19 & 20 Heat and te First Law of Termodynamics Te Zerot Law of Termodynamics Te First Law of Termodynamics Termal Processes Te Second Law of Termodynamics Heat Engines and te Carnot Cycle Refrigerators,

More information

1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity

1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity AP Physics Multiple Choice Practice Electrostatics 1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity. A soli conucting sphere is given a positive charge Q.

More information

Derivatives of trigonometric functions

Derivatives of trigonometric functions Derivatives of trigonometric functions 2 October 207 Introuction Toay we will ten iscuss te erivates of te si stanar trigonometric functions. Of tese, te most important are sine an cosine; te erivatives

More information

E p = mgh (if h i=0) E k = ½ mv 2 Ek is measured in Joules (J); m is measured in kg; v is measured in m/s. Energy Continued (E)

E p = mgh (if h i=0) E k = ½ mv 2 Ek is measured in Joules (J); m is measured in kg; v is measured in m/s. Energy Continued (E) nergy Continued () Gravitational Potential nergy: - e energy stored in an object due to its distance above te surface of te art. - e energy stored depends on te mass of te object, te eigt above te surface,

More information

Work and Energy. Introduction. Work. PHY energy - J. Hedberg

Work and Energy. Introduction. Work. PHY energy - J. Hedberg Work and Energy PHY 207 - energy - J. Hedberg - 2017 1. Introduction 2. Work 3. Kinetic Energy 4. Potential Energy 5. Conservation of Mecanical Energy 6. Ex: Te Loop te Loop 7. Conservative and Non-conservative

More information

MVT and Rolle s Theorem

MVT and Rolle s Theorem AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state

More information

Journal of Engineering Science and Technology Review 7 (4) (2014) 40-45

Journal of Engineering Science and Technology Review 7 (4) (2014) 40-45 Jestr Journal of Engineering Science and Tecnology Review 7 (4) (14) -45 JOURNAL OF Engineering Science and Tecnology Review www.jestr.org Mecanics Evolution Caracteristics Analysis of in Fully-mecanized

More information

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as . Derivative. Definition of Derivative at a Point: Te derivative of te function f at a is defined as f fa fa a lim provided te limit eists. If te limit eists, we sa tat f is differentiable at a, oterwise,

More information

Grade: 11 International Physics Olympiad Qualifier Set: 2

Grade: 11 International Physics Olympiad Qualifier Set: 2 Grade: 11 International Pysics Olympiad Qualifier Set: 2 --------------------------------------------------------------------------------------------------------------- Max Marks: 60 Test ID: 12111 Time

More information

Notes on the function gsw_enthalpy_first_derivatives_ct_exact(sa,ct,p)

Notes on the function gsw_enthalpy_first_derivatives_ct_exact(sa,ct,p) Notes on gsw_entaly_first_derivatives_c_exact 1 Notes on te function gsw_entaly_first_derivatives_c_exact(c) is function gsw_entaly_first_derivatives_c_exact(c) evaluates two of te first order artial derivatives

More information

A NEW INTERPRETATION OF PHOTON. Kunwar Jagdish Narain

A NEW INTERPRETATION OF PHOTON. Kunwar Jagdish Narain 1 A NW INTRPRTATION OF PHOTON a) b) Kunwar Jagdis Narain (Retired Professor of Pysics) Te resent interretation of oton is as: A oton = a quantum of radiation energy + energy, were te quantum of radiation

More information

Outline. MS121: IT Mathematics. Limits & Continuity Rates of Change & Tangents. Is there a limit to how fast a man can run?

Outline. MS121: IT Mathematics. Limits & Continuity Rates of Change & Tangents. Is there a limit to how fast a man can run? Outline MS11: IT Matematics Limits & Continuity & 1 Limits: Atletics Perspective Jon Carroll Scool of Matematical Sciences Dublin City University 3 Atletics Atletics Outline Is tere a limit to ow fast

More information

Mathematics 123.3: Solutions to Lab Assignment #5

Mathematics 123.3: Solutions to Lab Assignment #5 Matematics 3.3: Solutions to Lab Assignment #5 Find te derivative of te given function using te definition of derivative. State te domain of te function and te domain of its derivative..: f(x) 6 x Solution:

More information

Hong Xu. School of Business and Management, Hong Kong University of Science and Technology, Clearwater Bay, Kowloon, HONG KONG

Hong Xu. School of Business and Management, Hong Kong University of Science and Technology, Clearwater Bay, Kowloon, HONG KONG RESEARCH ARTICLE IDETITY MAAGEMET AD TRADABLE REPUTATIO Hong Xu Scoo of Business an Management, Hong Kong University of Science an Tecnoogy, Cearater Bay, Kooon, HOG KOG {xu@ust.} Jianqing Cen Jina Scoo

More information

PhyzExamples: Advanced Electrostatics

PhyzExamples: Advanced Electrostatics PyzExaples: Avance Electrostatics Pysical Quantities Sybols Units Brief Definitions Carge or Q coulob [KOO lo]: C A caracteristic of certain funaental particles. Eleentary Carge e 1.6 10 19 C Te uantity

More information

Numerical Simulations of the Physical Process for Hailstone Growth

Numerical Simulations of the Physical Process for Hailstone Growth NO.1 FANG Wen, ZHENG Guoguang and HU Zijin 93 Numerical Simulations of te Pysical Process for Hailstone Growt FANG Wen 1,3 ( ), ZHENG Guoguang 2 ( ), and HU Zijin 3 ( ) 1 Nanjing University of Information

More information

The isentropic exponent in plasmas

The isentropic exponent in plasmas Te isentroic exonent in lasmas Burm K.T.A.L.; Goedeer W.J.; cram D.C. Publised in: Pysics of Plasmas DOI: 10.1063/1.873535 Publised: 01/01/1999 Document Version Publiser s PDF also known as Version of

More information

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator

Simulation and verification of a plate heat exchanger with a built-in tap water accumulator Simulation and verification of a plate eat excanger wit a built-in tap water accumulator Anders Eriksson Abstract In order to test and verify a compact brazed eat excanger (CBE wit a built-in accumulation

More information

Wireless Communications

Wireless Communications Wireless Communications Cannel Moeling Large Scale Hami Barami Electrical & Computer Engineering EM Spectrum Raio Wave l Raio wave: a form of electromagnetic raiation, create wenever a carge object accelerates

More information

Path to static failure of machine components

Path to static failure of machine components Pat to static failure of macine components Load Stress Discussed last week (w) Ductile material Yield Strain Brittle material Fracture Fracture Dr. P. Buyung Kosasi,Spring 008 Name some of ductile and

More information

Sample Problems for Exam II

Sample Problems for Exam II Sample Problems for Exam 1. Te saft below as lengt L, Torsional stiffness GJ and torque T is applied at point C, wic is at a distance of 0.6L from te left (point ). Use Castigliano teorem to Calculate

More information

Soil Plasticity and the Structured Cam Clay Model

Soil Plasticity and the Structured Cam Clay Model Soil Plasticity an the Structure Cam Clay Moel Dr. Martin D. Liu School of Ciil Engineering Uniersity of New South Wales Syney, NSW 2052, Australia Tel.: 2-9385-5474 Fax: 2-9385-639 e-mail: martin.liu@unsw.eu.au

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information

Performance analysis of Carbon Nano Tubes

Performance analysis of Carbon Nano Tubes IOSR Journal of Engineering (IOSRJEN) ISSN: 2250-3021 Volume 2, Issue 8 (August 2012), PP 54-58 Performance analysis of Carbon Nano Tubes P.S. Raja, R.josep Daniel, Bino. N Dept. of E & I Engineering,

More information

The Effects of Mutual Coupling and Transformer Connection Type on Frequency Response of Unbalanced Three Phase Electrical Distribution System

The Effects of Mutual Coupling and Transformer Connection Type on Frequency Response of Unbalanced Three Phase Electrical Distribution System Energy an Power Engineering, 00,, 8-47 oi:0.46/epe.00.405 Publise Online November 00 (ttp://www.scirp.org/journal/epe) Te Effects of Mutual Coupling an Transformer Connection Type on Frequency Response

More information

NCCI: Simple methods for second order effects in portal frames

NCCI: Simple methods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames NCC: Simple metods for second order effects in portal frames Tis NCC presents information

More information

Differential Calculus Definitions, Rules and Theorems

Differential Calculus Definitions, Rules and Theorems Precalculus Review Differential Calculus Definitions, Rules an Teorems Sara Brewer, Alabama Scool of Mat an Science Functions, Domain an Range f: X Y a function f from X to Y assigns to eac x X a unique

More information

6. Non-uniform bending

6. Non-uniform bending . Non-uniform bending Introduction Definition A non-uniform bending is te case were te cross-section is not only bent but also seared. It is known from te statics tat in suc a case, te bending moment in

More information

Chapter 11: Relation between vorticity, divergence and the vertical velocity

Chapter 11: Relation between vorticity, divergence and the vertical velocity Cater 11: Relation between ticity, diergence and te ertical elocity Te diergence equation In cater 3 we used a simle ersion of te continuity equation. Here we deelo it furter, artly because it will gie

More information

Field-Observation Analysis of Sea-Bottom Effects on Thermal Environments in a Coral Reef

Field-Observation Analysis of Sea-Bottom Effects on Thermal Environments in a Coral Reef iel-observation Analysis of Sea-Bottom Effects on Termal Environments in a Coral Reef Yasuo Niei 1, Kazuo Naaoka, Yasuo Tsunasima 1, Yasunori Aoki 1 an Kensui Wakaki 1 Department of Civil Engineering,

More information

ON THE HEIGHT OF MAXIMUM SPEED-UP IN ATMOSPHERIC BOUNDARY LAYERS OVER LOW HILLS

ON THE HEIGHT OF MAXIMUM SPEED-UP IN ATMOSPHERIC BOUNDARY LAYERS OVER LOW HILLS ON THE HEIGHT OF MAXIMUM SPEED-UP IN ATMOSPHERIC BOUNDARY LAYERS OVER LOW HILLS Cláudio C. Pellegrini FUNREI Departamento de Ciências Térmicas e dos Fluidos Praça Frei Orlando 17, São João del-rei, MG,

More information

Chapter 1 Functions and Graphs. Section 1.5 = = = 4. Check Point Exercises The slope of the line y = 3x+ 1 is 3.

Chapter 1 Functions and Graphs. Section 1.5 = = = 4. Check Point Exercises The slope of the line y = 3x+ 1 is 3. Capter Functions and Graps Section. Ceck Point Exercises. Te slope of te line y x+ is. y y m( x x y ( x ( y ( x+ point-slope y x+ 6 y x+ slope-intercept. a. Write te equation in slope-intercept form: x+

More information

5. THERMAL CONVERSION OF SOLAR RADIATION. Content

5. THERMAL CONVERSION OF SOLAR RADIATION. Content 5. Introuction 5. THEMAL CONVESION OF SOLA ADIATION Content 5. Introuction 5. Collectors without concentration 5.. Otical efficiency of the flat collector 5.. Thermal efficiency of the flat collector 5..3

More information

Measurement of the heat transfer coefficient in the dimpled channel: effects of dimple arrangement and channel height

Measurement of the heat transfer coefficient in the dimpled channel: effects of dimple arrangement and channel height Journal of Mecanical Science and Tecnology 3 (009) 64~630 Journal of Mecanical Science and Tecnology www.sringerlink.com/content/738-494x DOI 0.007/s06-008-- Measurement of te eat transfer coefficient

More information

Problem Set 2: Solutions

Problem Set 2: Solutions UNIVERSITY OF ALABAMA Department of Physics an Astronomy PH 102 / LeClair Summer II 2010 Problem Set 2: Solutions 1. The en of a charge rubber ro will attract small pellets of Styrofoam that, having mae

More information

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4)

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4) Pysics Teac Yourself Series Topic 15: Wavelie nature of atter (Unit 4) A: Level 14, 474 Flinders Street Melbourne VIC 3000 T: 1300 134 518 W: tss.co.au E: info@tss.co.au TSSM 2017 Page 1 of 8 Contents

More information

Higher Derivatives. Differentiable Functions

Higher Derivatives. Differentiable Functions Calculus 1 Lia Vas Higer Derivatives. Differentiable Functions Te second derivative. Te derivative itself can be considered as a function. Te instantaneous rate of cange of tis function is te second derivative.

More information

Fabric Evolution and Its Effect on Strain Localization in Sand

Fabric Evolution and Its Effect on Strain Localization in Sand Fabric Evolution and Its Effect on Strain Localization in Sand Ziwei Gao and Jidong Zao Abstract Fabric anisotropy affects importantly te overall beaviour of sand including its strengt and deformation

More information

Convergence Analysis of Terminal ILC in the z Domain

Convergence Analysis of Terminal ILC in the z Domain 25 American Control Conference June 8-, 25 Portlan, OR, USA WeA63 Convergence Analysis of erminal LC in the Domain Guy Gauthier, an Benoit Boulet, Member, EEE Abstract his aer shows how we can aly -transform

More information

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible. 004 Algebra Pretest answers and scoring Part A. Multiple coice questions. Directions: Circle te letter ( A, B, C, D, or E ) net to te correct answer. points eac, no partial credit. Wic one of te following

More information

The derivative of a function f is a new function defined by. f f (x + h) f (x)

The derivative of a function f is a new function defined by. f f (x + h) f (x) Derivatives Definition Te erivative of a function f is a new function efine by f f (x + ) f (x) (x). 0 We will say tat a function f is ifferentiable over an interval (a, b) if if te erivative function

More information

Available online at ScienceDirect. Procedia Engineering 144 (2016 )

Available online at   ScienceDirect. Procedia Engineering 144 (2016 ) Available online at www.sciencedirect.com ScienceDirect Procedia Engineering (06 ) 03 030 t International onference on Vibration Problems, IOVP 05 Termal stresses, deformations and vibrations of lates

More information

CALCULATION OF COLLAPSE PRESSURE IN SHALE GAS FORMATION AND THE INFLUENCE OF FORMATION ANISOTROPY

CALCULATION OF COLLAPSE PRESSURE IN SHALE GAS FORMATION AND THE INFLUENCE OF FORMATION ANISOTROPY CALCULATION OF COLLAPSE PRESSURE IN SHALE GAS FORMATION AND THE INFLUENCE OF FORMATION ANISOTROPY L.Hu, J.Deng, F.Deng, H.Lin, C.Yan, Y.Li, H.Liu, W.Cao (Cina University of Petroleum) Sale gas formations

More information

INTRODUCTION & PHASE SYSTEM

INTRODUCTION & PHASE SYSTEM INTRODUCTION & PHASE SYSTEM Dr. Professor of Civil Engineering S. J. College of Engineering, Mysore 1.1 Geotechnical Engineering Why? 1. We are unable to buil castles in air (yet)! 2. Almost every structure

More information

the first derivative with respect to time is obtained by carefully applying the chain rule ( surf init ) T Tinit

the first derivative with respect to time is obtained by carefully applying the chain rule ( surf init ) T Tinit .005 ermal Fluids Engineering I Fall`08 roblem Set 8 Solutions roblem ( ( a e -D eat equation is α t x d erfc( u du π x, 4αt te first derivative wit respect to time is obtained by carefully applying te

More information

Damage Identification of a Long-Span Suspension Bridge Using Temperature- Induced Strain Data. Southeast University, Nanjing, China, ABSTRACT

Damage Identification of a Long-Span Suspension Bridge Using Temperature- Induced Strain Data. Southeast University, Nanjing, China, ABSTRACT Damage Identification of a Long-Span Suspension Bridge Using Temperature- Induced Strain Data *Qi. Xia 1) and Jian. Zang 2) 1 Scool of civil engineering, Souteast University, Nanjing, Cina 2 Key Laboratory

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

1 2 x Solution. The function f x is only defined when x 0, so we will assume that x 0 for the remainder of the solution. f x. f x h f x.

1 2 x Solution. The function f x is only defined when x 0, so we will assume that x 0 for the remainder of the solution. f x. f x h f x. Problem. Let f x x. Using te definition of te derivative prove tat f x x Solution. Te function f x is only defined wen x 0, so we will assume tat x 0 for te remainder of te solution. By te definition of

More information

1 ode.mcd. Find solution to ODE dy/dx=f(x,y). Instructor: Nam Sun Wang

1 ode.mcd. Find solution to ODE dy/dx=f(x,y). Instructor: Nam Sun Wang Fin solution to ODE /=f(). Instructor: Nam Sun Wang oe.mc Backgroun. Wen a sstem canges wit time or wit location, a set of ifferential equations tat contains erivative terms "/" escribe suc a namic sstem.

More information

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential

dn i where we have used the Gibbs equation for the Gibbs energy and the definition of chemical potential Chem 467 Sulement to Lectures 33 Phase Equilibrium Chemical Potential Revisited We introduced the chemical otential as the conjugate variable to amount. Briefly reviewing, the total Gibbs energy of a system

More information

MATH 111 CHAPTER 2 (sec )

MATH 111 CHAPTER 2 (sec ) MATH CHAPTER (sec -0) Terms to know: function, te domain and range of te function, vertical line test, even and odd functions, rational power function, vertical and orizontal sifts of a function, reflection

More information

Thermoelastic Buckling Analysis of Power-law, Sigmoid, Exponential FGM Circular Plates with Piezoelectric Actuators

Thermoelastic Buckling Analysis of Power-law, Sigmoid, Exponential FGM Circular Plates with Piezoelectric Actuators 3rd International Conference on Mecanical, Electronics and Mecatronics Engineering (ICMEME'4) Marc 9-, 4 Abu Dabi (UAE) ermoelastic Buckling Analysis of Power-law, Sigmoid, Exonential FGM Circular Plates

More information

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2

Physics 121, April 1, Equilibrium. Physics 121. April 1, Physics 121. April 1, Course Information. Discussion of Exam # 2 Pysics 121, April 1, 2008. Pysics 121. April 1, 2008. Course Information Discussion of Exam # 2 Topics to be discussed today: Requirements for Equilibrium Gravitational Equilibrium Sample problems Pysics

More information

FOCUS ON THEORY. We recall that a function g(x) is differentiable at the point a if the limit

FOCUS ON THEORY. We recall that a function g(x) is differentiable at the point a if the limit FOCUS ON THEORY 653 DIFFERENTIABILITY Notes on Differentiabilit In Section 13.3 we gave an informal introduction to te concet of differentiabilit. We called a function f (; ) differentiable at a oint (a;

More information

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln

Section A 01. (12 M) (s 2 s 3 ) = 313 s 2 = s 1, h 3 = h 4 (s 1 s 3 ) = kj/kgk. = kj/kgk. 313 (s 3 s 4f ) = ln 0. (a) Sol: Section A A refrigerator macine uses R- as te working fluid. Te temperature of R- in te evaporator coil is 5C, and te gas leaves te compressor as dry saturated at a temperature of 40C. Te mean

More information

Pumping Heat with Quantum Ratchets

Pumping Heat with Quantum Ratchets Pumping Heat wit Quantum Ratcets T. E. Humprey a H. Linke ab R. Newbury a a Scool of Pysics University of New Sout Wales UNSW Sydney 5 Australia b Pysics Department University of Oregon Eugene OR 9743-74

More information

Keywords: pile, liquefaction, lateral spreading, analysis ABSTRACT

Keywords: pile, liquefaction, lateral spreading, analysis ABSTRACT Key arameters in seudo-static analysis of iles in liquefying sand Misko Cubrinovski Deartment of Civil Engineering, University of Canterbury, Christchurch 814, New Zealand Keywords: ile, liquefaction,

More information

Krazy Katt, the mechanical cat

Krazy Katt, the mechanical cat Krazy Katt, te mecanical cat Te cat rigting relex is a cat's innate ability to orient itsel as it alls in order to land on its eet. Te rigting relex begins to appear at 3 4 weeks o age, and is perected

More information

MATH 3208 MIDTERM REVIEW. (B) {x 4 x 5 ; x ʀ} (D) {x x ʀ} Use the given functions to answer questions # 3 5. determine the value of h(7).

MATH 3208 MIDTERM REVIEW. (B) {x 4 x 5 ; x ʀ} (D) {x x ʀ} Use the given functions to answer questions # 3 5. determine the value of h(7). MATH 08 MIDTERM REVIEW. If () = (f + g)() wat is te domain of () { 5 4 ; ʀ} { 4 4 ; ʀ} { 4 5 ; ʀ} { ʀ}. Given p() = and g() = wic function represents k() k() = p() g() + + Use te given functions to answer

More information

Math 34A Practice Final Solutions Fall 2007

Math 34A Practice Final Solutions Fall 2007 Mat 34A Practice Final Solutions Fall 007 Problem Find te derivatives of te following functions:. f(x) = 3x + e 3x. f(x) = x + x 3. f(x) = (x + a) 4. Is te function 3t 4t t 3 increasing or decreasing wen

More information

ECE 422 Power System Operations & Planning 7 Transient Stability

ECE 422 Power System Operations & Planning 7 Transient Stability ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of

More information

3. Using your answers to the two previous questions, evaluate the Mratio

3. Using your answers to the two previous questions, evaluate the Mratio MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING CAMBRIDGE, MASSACHUSETTS 0219 2.002 MECHANICS AND MATERIALS II HOMEWORK NO. 4 Distributed: Friday, April 2, 2004 Due: Friday,

More information

The Derivative The rate of change

The Derivative The rate of change Calculus Lia Vas Te Derivative Te rate of cange Knowing and understanding te concept of derivative will enable you to answer te following questions. Let us consider a quantity wose size is described by

More information

Sedimentation. Treatment Processes. Sedimentation. Sedimentation. Sedimentation. Sedimentation. CIVL 1112 Water Treatment - Sedimentation 1/7

Sedimentation. Treatment Processes. Sedimentation. Sedimentation. Sedimentation. Sedimentation. CIVL 1112 Water Treatment - Sedimentation 1/7 CIVL 111 Water Treatment - 1/7 Treatment Processes is te donards movement of an object relative to its surrounding medium, due to te force of gravity. Screening Aeration Preclorination locculation Coagulation

More information

A Simple Exchange Economy with Complex Dynamics

A Simple Exchange Economy with Complex Dynamics FH-Kiel Universitf Alie Sciences Prof. Dr. Anreas Thiemer, 00 e-mail: anreas.thiemer@fh-kiel.e A Simle Exchange Economy with Comlex Dynamics (Revision: Aril 00) Summary: Mukherji (999) shows that a stanar

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

Part 2: Introduction to Open-Channel Flow SPRING 2005

Part 2: Introduction to Open-Channel Flow SPRING 2005 Part : Introduction to Open-Cannel Flow SPRING 005. Te Froude number. Total ead and specific energy 3. Hydraulic jump. Te Froude Number Te main caracteristics of flows in open cannels are tat: tere is

More information

Free Vibration Analysis of a Model Structure with New Tuned Cradle Mass Damper

Free Vibration Analysis of a Model Structure with New Tuned Cradle Mass Damper Proc. Schl. Eng. Tokai Tokai Univ., Univ., Ser. ESer. E 37 (0) 37(0)3-8 3-8 Free Vibration Analysis of a Moel Structure with New Tune Crale Mass Damer by Jitjinakun AMONPHAN * an Yoji SHIMAZAKI * (Receive

More information