Van Der Waals Constants k b = 1.38 x J K -1 Substance. Substance

Size: px
Start display at page:

Download "Van Der Waals Constants k b = 1.38 x J K -1 Substance. Substance"

Transcription

1 Cheistry 45 Physial Cheistry I Exa I Given Info: R 8.35 J ol - K - Van Der Waals Constants k b.38 x 0-3 J K - Substane a b P T (J. 3 /ole ) ( 3 /ole) (MPa) (K) Air x K Carbon Dioxide (CO ) x K Nitrogen (N ) x K Hydrogen (H ) x K Water (H O) x K Aonia (NH 3 ) x K Heliu (He) x K Freon (CCl F ) x K A 0 a B 0 b Pa 6 ol ol ol ol ol - He Ne Ar H N O Air CO CH Substane

2 . No one an ever say I didn t ake you plug and hug a. For 0.53 oles of CO in a.5l vessel at 300K, assuing the Beattie- Bridgan value for the pressure is the true value, what is the perent error given by the Ideal Gas equation and by Van Der Waals? V.5/ L/ol /ol Beattie-Bridgean A (-7.3 x 0-6 /0.0083) B x 0-6 (-7.35 x 0-6 /0.0083).008 x P ( x0 ) N Ideal P RT/V 8.35*300/ N - Van Der Waals N 5 P x % error Ideal ( 00) 4.49% % error VDW ( ) 0.70% b. What is u for O at 300K? u 3RT x0 s M If I said that Fred and Wila, on average, were oving at.3 /s and 6.77 /s respetively at the sae teperature, then what is the ratio of their asses? u M so we an say that u u W F M 6.77 F. Fro here, 6. 3 M W.3

3 d. Ok, so let s say, for the sake of arguent, that He is an ideal gas. I deide to put a ole of it in an expandable vessel and do a ouple things. First, I inrease the pressure real fast like fro 4 Pa to 63 Pa at 73 K. What is the agnitude of the work here? Is work being done on the gas or is it doing work on e? Now, being real exited about that result, I deide to sit for infinity and perfor the experient again over that period of tie. What is the agnitude of the work now? What perentage of the energy I observed the seond tie was not seen the first tie? V nrt/p (8.35)(73)/4 6 3 and siilarly, V 36 3 w irr -P (V V ) -4(36 6) 764 J/ol work done on syste w rev V V PdV nrt V V dv V V nrt ln V ln J ol Finally, the perent not seen the first tie is ( )/344*00 48%

4 . Now to business. Modeling! I put a bunh of ants on the floor of a very thin tank. The tank is sloped downhill as shown. I then put soe haburger at the top of the slope. This generates a tendeny for the ants to ove towards the food, but this tendeny is biased by gravity. Now soe ants are hungrier than others and have ore drive to reah the food. Soe are repulsed by the food (vegetarians), and soe are indifferent to it. This eans that the ants are not experiening this situation equally, in fat, one ould desribe the fore that drives their position at a given tie along the line ab as a distribution. Ok, so let s define their drive to reah the food as z and the ants are experiening a distribution, φ, of drive at a snapshot in tie as the following: g a eat 60 o 30 o z b φ ( z ) σ e π ( z z0 ) ( )dz σ This happy equation ay be failiar to soe of you. It is the forula for a bell urve with z o being the average value of z and σ being the standard deviation. Ok, so a given ant has z for its drive. Now the fore experiened by eah ant is siple: F ant z - F g These are diretional fores, but we are only onerned with the diretion along the floor of the tank so they an be treated as salars using only sign to designate diretion. With this in ind, let s start the proble a. What is the fore experiened by eah ant due to gravity along the floor of the box. (Hint: this should be parallel to and in the opposite diretion of the arrow z above) g 60 o F g The diagra to the right desribes the situation. F g is the projetion of gravity along the botto of the tank. F g g osθ ½ g b. The ass of an ant is. What is the total fore experiened by eah ant along the floor of the tank? F ant z - ½ g

5 . In ters of variables only, what fration of ants are oving towards the food? (Only set this one up, I want to see all the relevant paraeters) The ant is oving towards the food for all values of z that are greater than the fore fro gravity. Matheatially, this is when z > ½ g. the distribution of the values of z is represented by φ(z) so the final expression is f g z> g φ ( z) ( z z ) 0 σ σ π g e dz 3. a. If the ratio of P /P / and the ratio of V /V /3, then what is T if T 98 K? ( PV ) T ( P V ) T 3 T 98 T 788 K b. For substane above, the virial oeffiients are desribed as the following: b i 3 X T i T T where b - i- ( ) i i For V, at what values for T does the gas behave ideally? (use the seond, third and fourth virial oeffiients) For V, Z + B(T) + C(T) + D(T) + ½ T - T + 3 T 3 + ¼ T T 4 so the gas will behave ideally for all roots of ½ T - T + 3 T 3 + ¼ T T 4 0 this has two roots at T 0 and two ore roots defined by ½ T T + ¼ T T 0 we an find quadrati roots by the quadrati forula: T 3 ± 9 4 T 4 T 3T ± , 536 T All this to say that these roots are not physial reality, so the only plae where this gas would behave ideally is at T 0.

6 4. Given this relationship: (not a real relationship, treat it as ideal) U ( T ) V lnt Using only relationships derived last week, give expressions for the following in ters of R and P: C V, C du dt V V, V, T R P C P, (do not use C p, C v, + R) C dh and H U + RT V lnt + RT RT/P ln T + RT P, dt P, so C dh R R lnt + dt P P P, + P, R Finally, derive a relationship between C P, and C V,. Should this gas be treated as ideal? If C V, R/P then CP, CV, ln T + CV, + R whih is different fro the ideal relationship, C P, C V, + R, so it should not be treated as ideal.

Problem Set 2. Chapter 1 Numerical:

Problem Set 2. Chapter 1 Numerical: Chapter 1 Nuerical: roble Set 16. The atoic radius of xenon is 18 p. Is that consistent with its b paraeter of 5.15 1 - L/ol? Hint: what is the volue of a ole of xenon atos and how does that copare to

More information

Chemistry Department Al-kharj, October Prince Sattam Bin Abdulaziz University First semester (1437/1438)

Chemistry Department Al-kharj, October Prince Sattam Bin Abdulaziz University First semester (1437/1438) Exercise 1 Exercises- chapter-1- Properties of gases (Part-2- Real gases Express the van der Waals paraeters a = 1.32 at d 6 ol 2 and b = 0.0436 d 3 ol 1 in SI base units? * The SI unit of pressure is

More information

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30.

All Excuses must be taken to 233 Loomis before 4:15, Monday, April 30. Miscellaneous Notes he end is near don t get behind. All Excuses ust be taken to 233 Loois before 4:15, Monday, April 30. he PHYS 213 final exa ties are * 8-10 AM, Monday, May 7 * 8-10 AM, uesday, May

More information

I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class.

I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class. Che340 hysical Cheistry for Biocheists Exa 3 Apr 5, 0 Your Nae _ I affir that I have never given nor received aid on this exaination. I understand that cheating in the exa will result in a grade F for

More information

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along (40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass

More information

OStudy of Real Gas Behavior: Ideality of CO 2 Gas

OStudy of Real Gas Behavior: Ideality of CO 2 Gas OStudy of Real Gas Behavior: Ideality of CO Gas Subitted: March, 014 CHEM 457, Section Departent of Cheistry, The Pennsylvania State University, University Park, PA 1680 Jessica Slavejkov Bashayer Aldakkan,

More information

21. Practice Problem (page 556) What is the volume of 5.65 mol of helium gas at a pressure of 98 kpa and a temperature of 18.0 C?

21. Practice Problem (page 556) What is the volume of 5.65 mol of helium gas at a pressure of 98 kpa and a temperature of 18.0 C? Section 12.2 The Ideal Gas Law Solutions for Practice Probles Student Edition page 556 21. Practice Proble (page 556) What is the volue of 5.65 ol of heliu gas at a pressure of 98 kpa and a teperature

More information

1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the

1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the . Whih two values of teperature are equivalent to the nearest degree when easured on the Kelvin and on the Celsius sales of teperature? Kelvin sale Celsius sale A. 40 33 B. 273 00 C. 33 40 D. 373 0 2.

More information

Physical Chemistry I for Biochemists. Lecture 2 (1/12/11) Yoshitaka Ishii. Gas Ch. 1 Non-Ideal Gas (Ch 1 & Raff p21-41) Announcement

Physical Chemistry I for Biochemists. Lecture 2 (1/12/11) Yoshitaka Ishii. Gas Ch. 1 Non-Ideal Gas (Ch 1 & Raff p21-41) Announcement Physical Cheistry I for Biocheists Che340 Lecture (1/1/11) Yoshitaka Ishii Gas Ch. 1 No-Ideal Gas (Ch 1 & Raff p1-41) Aouceet HW 1 is due et Wedesday before the class (Fid HW1 at the web site) Attedace

More information

Scholarship Calculus (93202) 2013 page 1 of 8. ( 6) ± 20 = 3± 5, so x = ln( 3± 5) 2. 1(a) Expression for dy = 0 [1st mark], [2nd mark], width is

Scholarship Calculus (93202) 2013 page 1 of 8. ( 6) ± 20 = 3± 5, so x = ln( 3± 5) 2. 1(a) Expression for dy = 0 [1st mark], [2nd mark], width is Sholarship Calulus 93) 3 page of 8 Assessent Shedule 3 Sholarship Calulus 93) Evidene Stateent Question One a) e x e x Solving dy dx ln x x x ln ϕ e x e x e x e x ϕ, we find e x x e y The drop is widest

More information

Answers to assigned problems from Chapter 1

Answers to assigned problems from Chapter 1 Answers to assigned probles fro Chapter 1 1.7. a. A colun of ercury 1 in cross-sectional area and 0.001 in height has a volue of 0.001 and a ass of 0.001 1 595.1 kg. Then 1 Hg 0.001 1 595.1 kg 9.806 65

More information

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016 NB1140: Physics 1A - Classical echanics and Therodynaics Proble set 2 - Forces and energy Week 2: 21-25 Noveber 2016 Proble 1. Why force is transitted uniforly through a assless string, a assless spring,

More information

Question 1. [14 Marks]

Question 1. [14 Marks] 6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is

More information

U V. r In Uniform Field the Potential Difference is V Ed

U V. r In Uniform Field the Potential Difference is V Ed SPHI/W nit 7.8 Electric Potential Page of 5 Notes Physics Tool box Electric Potential Energy the electric potential energy stored in a syste k of two charges and is E r k Coulobs Constant is N C 9 9. E

More information

Physics 2107 Oscillations using Springs Experiment 2

Physics 2107 Oscillations using Springs Experiment 2 PY07 Oscillations using Springs Experient Physics 07 Oscillations using Springs Experient Prelab Read the following bacground/setup and ensure you are failiar with the concepts and theory required for

More information

Problem T1. Main sequence stars (11 points)

Problem T1. Main sequence stars (11 points) Proble T1. Main sequence stars 11 points Part. Lifetie of Sun points i..7 pts Since the Sun behaves as a perfectly black body it s total radiation power can be expressed fro the Stefan- Boltzann law as

More information

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces

More information

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2! Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In

More information

TAP 702-6: Binary stars

TAP 702-6: Binary stars TAP 702-6: Binary stars Orbiting binary stars: A type of ariable star. This type of ariable star onsists of two stars orbiting around eah other. When the dier star is in front of the brighter one, the

More information

26 Impulse and Momentum

26 Impulse and Momentum 6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction

More information

Lecture 23: Spinodal Decomposition: Part 2: regarding free energy. change and interdiffusion coefficient inside the spinodal

Lecture 23: Spinodal Decomposition: Part 2: regarding free energy. change and interdiffusion coefficient inside the spinodal Leture 3: Spinodal eoposition: Part : regarding free energy hange and interdiffusion oeffiient inside the spinodal Today s topis ontinue to understand the basi kinetis of spinodal deoposition. Within the

More information

Introduction to Robotics (CS223A) (Winter 2006/2007) Homework #5 solutions

Introduction to Robotics (CS223A) (Winter 2006/2007) Homework #5 solutions Introduction to Robotics (CS3A) Handout (Winter 6/7) Hoework #5 solutions. (a) Derive a forula that transfors an inertia tensor given in soe frae {C} into a new frae {A}. The frae {A} can differ fro frae

More information

Definition of Work, The basics

Definition of Work, The basics Physics 07 Lecture 16 Lecture 16 Chapter 11 (Work) v Eploy conservative and non-conservative forces v Relate force to potential energy v Use the concept of power (i.e., energy per tie) Chapter 1 v Define

More information

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the Leture 4: Spinodal Deoposition: Part 3: kinetis of the oposition flutuation Today s topis Diffusion kinetis of spinodal deoposition in ters of the onentration (oposition) flutuation as a funtion of tie:

More information

ln P 1 saturation = T ln P 2 saturation = T

ln P 1 saturation = T ln P 2 saturation = T More Tutorial at www.littledubdoctor.co Physical Cheistry Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILY understand your

More information

Massachusetts Institute of Technology Quantum Mechanics I (8.04) Spring 2005 Solutions to Problem Set 4

Massachusetts Institute of Technology Quantum Mechanics I (8.04) Spring 2005 Solutions to Problem Set 4 Massachusetts Institute of Technology Quantu Mechanics I (8.04) Spring 2005 Solutions to Proble Set 4 By Kit Matan 1. X-ray production. (5 points) Calculate the short-wavelength liit for X-rays produced

More information

Expansion of Gases. It is decided to verify oyle's law over a wide range of teperature and pressures. he ost suitable gas to be selected for this purpose is ) Carbon dioxide ) Heliu 3) Oxygen 4) Hydrogen.

More information

1 The properties of gases The perfect gas

1 The properties of gases The perfect gas 1 The properties of gases 1A The perfect gas Answers to discussion questions 1A. The partial pressure of a gas in a ixture of gases is the pressure the gas would exert if it occupied alone the sae container

More information

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ). Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D

More information

Some Perspective. Forces and Newton s Laws

Some Perspective. Forces and Newton s Laws Soe Perspective The language of Kineatics provides us with an efficient ethod for describing the otion of aterial objects, and we ll continue to ake refineents to it as we introduce additional types of

More information

(Newton s 2 nd Law for linear motion)

(Newton s 2 nd Law for linear motion) PHYSICS 3 Final Exaination ( Deeber Tie liit 3 hours Answer all 6 questions You and an assistant are holding the (opposite ends of a long plank when oops! the butterfingered assistant drops his end If

More information

CHEM 305 Solutions for assignment #2

CHEM 305 Solutions for assignment #2 CHEM 05 Solutions for assignent #. (a) Starting fro C C show that C C Substitute the result into the original expression for C C : C C (b) Using the result fro (a), evaluate C C for an ideal gas. a. Both

More information

Note-A-Rific: Mechanical

Note-A-Rific: Mechanical Note-A-Rific: Mechanical Kinetic You ve probably heard of inetic energy in previous courses using the following definition and forula Any object that is oving has inetic energy. E ½ v 2 E inetic energy

More information

Shear Force and Bending Moment

Shear Force and Bending Moment Shear Fore and Bending oent Shear Fore: is the algebrai su of the vertial fores ating to the left or right of a ut setion along the span of the bea Bending oent: is the algebrai su of the oent of the fores

More information

MAE 110A. Homework 6: Solutions 11/9/2017

MAE 110A. Homework 6: Solutions 11/9/2017 MAE 110A Hoework 6: Solutions 11/9/2017 H6.1: Two kg of H2O contained in a piston-cylinder assebly, initially at 1.0 bar and 140 C undergoes an internally ersible, isotheral copression to 25 bar. Given

More information

ELEC NCERT. 1. Which cell will measure standard electrode potential of copper electrode? (g,0.1 bar) H + (aq.,1 M) Cu 2+ (aq.

ELEC NCERT. 1. Which cell will measure standard electrode potential of copper electrode? (g,0.1 bar) H + (aq.,1 M) Cu 2+ (aq. I. Multiple Choice Questions (Type-I) 1. Which cell will easure standard electrode potential of copper electrode? Pt (s) H 2 (g,0.1 bar) H + (aq.,1 M) Cu 2+ (aq.,1m) Cu Pt(s) H 2 (g, 1 bar) H + (aq.,1

More information

Part I: How Dense Is It? Fundamental Question: What is matter, and how do we identify it?

Part I: How Dense Is It? Fundamental Question: What is matter, and how do we identify it? Part I: How Dense Is It? Fundaental Question: What is atter, and how do we identify it? 1. What is the definition of atter? 2. What do you think the ter ass per unit volue eans? 3. Do you think that a

More information

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich TUTORIAL 1 SIMPLE HARMONIC MOTION Instructor: Kazui Tolich About tutorials 2 Tutorials are conceptual exercises that should be worked on in groups. Each slide will consist of a series of questions that

More information

8.1 Force Laws Hooke s Law

8.1 Force Laws Hooke s Law 8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which

More information

1. Simplify this circuit to find the total power absorbed by all resistors. R1 R3 47

1. Simplify this circuit to find the total power absorbed by all resistors. R1 R3 47 Hoework 1. iplify this iruit to find the total power asored y all resistors. R1 R 6 R4 0 47 R 47 Ans: Use series and parallel oinations to siplify iruit. R1R= 47 47 =94Ω and this resistane is in parallel

More information

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name:

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name: Che/Bioche 47 Exa /8/08 Pae of 7 Please leave the exa paes stapled toether. The forulas are on a separate sheet. This exa has 5 questions. You ust answer at least 4 of the questions. You ay answer ore

More information

PY241 Solutions Set 9 (Dated: November 7, 2002)

PY241 Solutions Set 9 (Dated: November 7, 2002) PY241 Solutions Set 9 (Dated: Noveber 7, 2002) 9-9 At what displaceent of an object undergoing siple haronic otion is the agnitude greatest for the... (a) velocity? The velocity is greatest at x = 0, the

More information

HW 6 - Solutions Due November 20, 2017

HW 6 - Solutions Due November 20, 2017 Conteporary Physics I HW 6 HW 6 - Solutions Due Noveber 20, 2017 1. A 4 kg block is attached to a spring with a spring constant k 200N/, and is stretched an aount 0.2 [5 pts each]. (a) Sketch the potential

More information

Tables of data and equations are on the last pages of the exam.

Tables of data and equations are on the last pages of the exam. Nae 4 August 2005 CHM 112 Final Exa (150 pts total) Tables of data and equations are on the last pages of the exa. (1.) Methanol (CH 3 OH) is anufactured by the reaction of carbon onoxide with hydrogen

More information

Daniel López Gaxiola 1 Student View Jason M. Keith

Daniel López Gaxiola 1 Student View Jason M. Keith Suppleental Material for Transport Process and Separation Process Principles Chapter Principles of Moentu Transfer and Overall Balances In fuel cells, the fuel is usually in gas or liquid phase. Thus,

More information

PHY 171. Lecture 14. (February 16, 2012)

PHY 171. Lecture 14. (February 16, 2012) PHY 171 Lecture 14 (February 16, 212) In the last lecture, we looked at a quantitative connection between acroscopic and icroscopic quantities by deriving an expression for pressure based on the assuptions

More information

Worked Solutions to Problems

Worked Solutions to Problems rd International Cheistry Olypiad Preparatory Probles Wored Solutions to Probles. Water A. Phase diagra a. he three phases of water oeist in equilibriu at a unique teperature and pressure (alled the triple

More information

ME 300 Thermodynamics II Exam 2 November 13, :00 p.m. 9:00 p.m.

ME 300 Thermodynamics II Exam 2 November 13, :00 p.m. 9:00 p.m. ME 300 Therodynaics II Exa 2 Noveber 3, 202 8:00 p.. 9:00 p.. Nae: Solution Section (Circle One): Sojka Naik :30 a.. :30 p.. Instructions: This is a closed book/notes exa. You ay use a calculator. You

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

Congruences and Modular Arithmetic

Congruences and Modular Arithmetic Congruenes and Modular Aritheti 6-17-2016 a is ongruent to b od n eans that n a b. Notation: a = b (od n). Congruene od n is an equivalene relation. Hene, ongruenes have any of the sae properties as ordinary

More information

Molecular interactions in beams

Molecular interactions in beams Molecular interactions in beas notable advanceent in the experiental study of interolecular forces has coe fro the developent of olecular beas, which consist of a narrow bea of particles, all having the

More information

points Points <40. Results of. Final Exam. Grade C D,F C B

points Points <40. Results of. Final Exam. Grade C D,F C B Results of inal Exa 5 6 7 8 9 points Grade C D, Points A 9- + 85-89 7-8 C + 6-69 -59 < # of students Proble (che. equilibriu) Consider the following reaction: CO(g) + H O(g) CO (g) + H (g) In equilibriu

More information

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE)

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE) The Lagrangian ethod vs. other ethods () This aterial written by Jozef HANC, jozef.hanc@tuke.sk Technical University, Kosice, Slovakia For Edwin Taylor s website http://www.eftaylor.co/ 6 January 003 The

More information

Kinetic Theory of Gases: Elementary Ideas

Kinetic Theory of Gases: Elementary Ideas Kinetic Theory of Gases: Eleentary Ideas 17th February 2010 1 Kinetic Theory: A Discussion Based on a Siplified iew of the Motion of Gases 1.1 Pressure: Consul Engel and Reid Ch. 33.1) for a discussion

More information

Experiment 2: Hooke s Law

Experiment 2: Hooke s Law COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance

More information

National 5 Summary Notes

National 5 Summary Notes North Berwick High School Departent of Physics National 5 Suary Notes Unit 3 Energy National 5 Physics: Electricity and Energy 1 Throughout the Course, appropriate attention should be given to units, prefixes

More information

Work, Energy and Momentum

Work, Energy and Momentum Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered

More information

Chapter VI: Motion in the 2-D Plane

Chapter VI: Motion in the 2-D Plane Chapter VI: Motion in the -D Plane Now that we have developed and refined our vector calculus concepts, we can ove on to specific application of otion in the plane. In this regard, we will deal with: projectile

More information

An Approximate Model for the Theoretical Prediction of the Velocity Increase in the Intermediate Ballistics Period

An Approximate Model for the Theoretical Prediction of the Velocity Increase in the Intermediate Ballistics Period An Approxiate Model for the Theoretical Prediction of the Velocity... 77 Central European Journal of Energetic Materials, 205, 2(), 77-88 ISSN 2353-843 An Approxiate Model for the Theoretical Prediction

More information

yields m 1 m 2 q 2 = (m 1 + m 2 )(m 1 q m 2 q 2 2 ). Thus the total kinetic energy is T 1 +T 2 = 1 m 1m 2

yields m 1 m 2 q 2 = (m 1 + m 2 )(m 1 q m 2 q 2 2 ). Thus the total kinetic energy is T 1 +T 2 = 1 m 1m 2 1 I iediately have 1 q 1 = f( q )q/ q and q = f( q )q/ q. Multiplying these equations by and 1 (respectively) and then subtracting, I get 1 ( q 1 q ) = ( + 1 )f( q )q/ q. The desired equation follows after

More information

REVIEW QUESTIONS Chapter 15

REVIEW QUESTIONS Chapter 15 hemistry 10 ANSWER EY REVIEW QUESTIONS hapter 15 1. A mixture of 0.10 mol of NO, 0.050 mol of H and 0.10 mol of HO is plaed in a 1.0-L flask and allowed to reah equilibrium as shown below: NO (g) + H (g)

More information

Kinetic Theory of Gases: Elementary Ideas

Kinetic Theory of Gases: Elementary Ideas Kinetic Theory of Gases: Eleentary Ideas 9th February 011 1 Kinetic Theory: A Discussion Based on a Siplified iew of the Motion of Gases 1.1 Pressure: Consul Engel and Reid Ch. 33.1) for a discussion of

More information

4 = (0.02) 3 13, = 0.25 because = 25. Simi-

4 = (0.02) 3 13, = 0.25 because = 25. Simi- Theore. Let b and be integers greater than. If = (. a a 2 a i ) b,then for any t N, in base (b + t), the fraction has the digital representation = (. a a 2 a i ) b+t, where a i = a i + tk i with k i =

More information

BALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass

BALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the

More information

In this chapter we will start the discussion on wave phenomena. We will study the following topics:

In this chapter we will start the discussion on wave phenomena. We will study the following topics: Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical

More information

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact

Physically Based Modeling CS Notes Spring 1997 Particle Collision and Contact Physically Based Modeling CS 15-863 Notes Spring 1997 Particle Collision and Contact 1 Collisions with Springs Suppose we wanted to ipleent a particle siulator with a floor : a solid horizontal plane which

More information

Distillation. The Continuous Column. Learning Outcomes. Recap - VLE for Meth H 2 O. Gavin Duffy School of Electrical Engineering DIT Kevin Street

Distillation. The Continuous Column. Learning Outcomes. Recap - VLE for Meth H 2 O. Gavin Duffy School of Electrical Engineering DIT Kevin Street Distillation The Continuous Colun Gavin Duffy School of Electrical Engineering DIT Kevin Street Learning Outcoes After this lecture you should be able to.. Describe how continuous distillation works List

More information

Number of extra papers used if any

Number of extra papers used if any Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa 1 Circle your instructor s last nae Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division (9:0): Choi Division

More information

Introduction to Biomedical Engineering. John D. Enderle, Susan M. Blanchard, Joseph D. Bronzino. Errata

Introduction to Biomedical Engineering. John D. Enderle, Susan M. Blanchard, Joseph D. Bronzino. Errata Introduction to Bioedical Engineering John D. Enderle, Susan M. Blanchard, Joseph D. Bronzino Errata Chapter 1 p. 24, line 38: Chapter 20 instead of Chapter 21 Chapter 3 p. 81, Electricity in the Eighteenth

More information

2. Electric Current. E.M.F. of a cell is defined as the maximum potential difference between the two electrodes of the

2. Electric Current. E.M.F. of a cell is defined as the maximum potential difference between the two electrodes of the 2. Electric Current The net flow of charges through a etallic wire constitutes an electric current. Do you know who carries current? Current carriers In solid - the electrons in outerost orbit carries

More information

Oxidation ReductionReactions. Hanson Activity 4 4 2/13/2013. What is the oxidation number the pure element S 8? Conclusion of ch 4

Oxidation ReductionReactions. Hanson Activity 4 4 2/13/2013. What is the oxidation number the pure element S 8? Conclusion of ch 4 Oxidation ReductionReactions Conclusion of ch 4 Hanson Activity 4 4 Discuss Key Questions 1 4 of Activity 4 4, page 68, with your partner for five minutes. The clicker quiz will commence at 8:50 AM sharp

More information

The Seesaw Mechanism

The Seesaw Mechanism The Seesaw ehanis By obert. Klauber www.quantufieldtheory.info 1 Bakground It ay see unusual to have suh low values for asses of neutrinos, when all other partiles like eletrons, quarks, et are uh heavier,

More information

Announcements. Review: Lorentz & velocity transformations (relativistic version of Galileo) Transformations (in 1D) Some examples

Announcements. Review: Lorentz & velocity transformations (relativistic version of Galileo) Transformations (in 1D) Some examples Announeents Reading for Monda: Chapter.6-. First Mid-ter is in das (Feb. 9 th, 7:30p). It will oer Chapters &. Reiew: Lorentz & eloit transforations (relatiisti ersion of Galileo) Transforations (in D)

More information

Chapter 10 Atmospheric Forces & Winds

Chapter 10 Atmospheric Forces & Winds Chapter 10 Atospheric Forces & Winds Chapter overview: Atospheric Pressure o Horizontal pressure variations o Station vs sea level pressure Winds and weather aps Newton s 2 nd Law Horizontal Forces o Pressure

More information

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018

x(t) y(t) c c F(t) F(t) EN40: Dynamics and Vibrations Homework 6: Forced Vibrations Due Friday April 5, 2018 EN40: Dynais and Vibrations Hoewor 6: Fored Vibrations Due Friday April 5, 2018 Shool of Engineering Brown University 1. The vibration isolation syste shown in the figure has =20g, = 19.8 N / = 1.259 Ns

More information

International Journal of Thermodynamics, Vol. 18, No. 1, P (2015). Sergey G.

International Journal of Thermodynamics, Vol. 18, No. 1, P (2015).   Sergey G. International Journal of Therodynais Vol. 8 No. P. 3-4 (5). http://dx.doi.org/.554/ijot.5343 Four-diensional equation of otion for visous opressible and harged fluid with regard to the aeleration field

More information

Answers to Assigned Problems from Chapter 2

Answers to Assigned Problems from Chapter 2 Answers to Assigned Problems from Chapter 2 2.2. 1 mol of ice has a volume of 18.01 g/0.9168 g cm 3 = 19.64 cm 3 1 mol of water has a volume of 18.01 g/0.9998 g cm 3 = 18.01 cm 3 V(ice water) = 1.63 cm

More information

Lesson 24: Newton's Second Law (Motion)

Lesson 24: Newton's Second Law (Motion) Lesson 24: Newton's Second Law (Motion) To really appreciate Newton s Laws, it soeties helps to see how they build on each other. The First Law describes what will happen if there is no net force. The

More information

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START Laboratory Section: Last Revised on Deceber 15, 2014 Partners Naes: Grade: EXPERIMENT 8 Electron Beas 0. Pre-Laboratory Work [2 pts] 1. Nae the 2 forces that are equated in order to derive the charge to

More information

Modeling of vibration systems

Modeling of vibration systems Modeling of vibration systes Atual syste Mae design deision Choose physial paraeters, hange or augent syste if neessary Physial odeling Mae siple approiations based on engineering judgeent Physial odel

More information

Temperature and Thermodynamics, Part II. Topics to be Covered

Temperature and Thermodynamics, Part II. Topics to be Covered Teperature and Therodynaics, Part II Topics to be Covered Profiles of Teperature in the Boundary Layer Potential teperature Adiabatic Lapse Rate Theral Stratification 1/8/17 Why are We Interested in Theral

More information

and ζ in 1.1)? 1.2 What is the value of the magnification factor M for system A, (with force frequency ω = ωn

and ζ in 1.1)? 1.2 What is the value of the magnification factor M for system A, (with force frequency ω = ωn EN40: Dynais and Vibrations Hoework 6: Fored Vibrations, Rigid Body Kineatis Due Friday April 7, 017 Shool of Engineering Brown University 1. Syste A in the figure is ritially daped. The aplitude of the

More information

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta

USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta 1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve

More information

Article 18: Incorporating the absolute-absolute spacetime and its underlying absolute-absolute intrinsic-intrinsic spacetime into physics. Part I.

Article 18: Incorporating the absolute-absolute spacetime and its underlying absolute-absolute intrinsic-intrinsic spacetime into physics. Part I. ar, 1 TH FUNDANTAL THORY... () ol. 1(3C) : Artile 18 Artile 18: Inorporating the absolute-absolute spaetie and its underlying absolute-absolute intrinsi-intrinsi spaetie into physis. Part I. A. O. Adekugbe

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please

More information

Chapter 4: Hypothesis of Diffusion-Limited Growth

Chapter 4: Hypothesis of Diffusion-Limited Growth Suary This section derives a useful equation to predict quantu dot size evolution under typical organoetallic synthesis conditions that are used to achieve narrow size distributions. Assuing diffusion-controlled

More information

Unit 14 Harmonic Motion. Your Comments

Unit 14 Harmonic Motion. Your Comments Today s Concepts: Periodic Motion Siple - Mass on spring Daped Forced Resonance Siple - Pendulu Unit 1, Slide 1 Your Coents Please go through the three equations for siple haronic otion and phase angle

More information

Name Period. What force did your partner s exert on yours? Write your answer in the blank below:

Name Period. What force did your partner s exert on yours? Write your answer in the blank below: Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:

More information

Department of Physics Preliminary Exam January 3 6, 2006

Department of Physics Preliminary Exam January 3 6, 2006 Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.

More information

DEPARTMENT OF ECONOMETRICS AND BUSINESS STATISTICS

DEPARTMENT OF ECONOMETRICS AND BUSINESS STATISTICS ISSN 1440-771X AUSTRALIA DEPARTMENT OF ECONOMETRICS AND BUSINESS STATISTICS An Iproved Method for Bandwidth Selection When Estiating ROC Curves Peter G Hall and Rob J Hyndan Working Paper 11/00 An iproved

More information

ENGI 3424 Engineering Mathematics Problem Set 1 Solutions (Sections 1.1 and 1.2)

ENGI 3424 Engineering Mathematics Problem Set 1 Solutions (Sections 1.1 and 1.2) ENGI 344 Engineering Matheatics Proble Set 1 Solutions (Sections 1.1 and 1.) 1. Find the general solution of the ordinary differential equation y 0 This ODE is not linear (due to the product y ). However,

More information

PY /005 Practice Test 1, 2004 Feb. 10

PY /005 Practice Test 1, 2004 Feb. 10 PY 205-004/005 Practice Test 1, 2004 Feb. 10 Print nae Lab section I have neither given nor received unauthorized aid on this test. Sign ature: When you turn in the test (including forula page) you ust

More information

CHAPTER ONE. Physics and the Life Sciences

CHAPTER ONE. Physics and the Life Sciences Solution anual for Physics for the Life Sciences 2nd Edition by Allang Link download full: http://testbankair.co/download/solution-anual-forphysics-for-the-life-sciences-2nd-edition-by-allang/ CHAPTER

More information

Tactics Box 2.1 Interpreting Position-versus-Time Graphs

Tactics Box 2.1 Interpreting Position-versus-Time Graphs 1D kineatic Retake Assignent Due: 4:32p on Friday, October 31, 2014 You will receive no credit for ites you coplete after the assignent is due. Grading Policy Tactics Box 2.1 Interpreting Position-versus-Tie

More information

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will

More information

AP Physics Thermodynamics Wrap-up

AP Physics Thermodynamics Wrap-up AP Physics herodynaics Wrap-up Here are your basic equations for therodynaics. here s a bunch of the. 3 his equation converts teperature fro Fahrenheit to Celsius. his is the rate of heat transfer for

More information

Humidity parameters. Saturation (equilibrium) vapor pressure Condensation balances evaporation

Humidity parameters. Saturation (equilibrium) vapor pressure Condensation balances evaporation uidity paraeters Saturation (equilibriu) vapor pressure Condensation balances evaporation Miing ratio & specific huidity Mass ratio of water vapor and air and water content and wet air. Dew point & frost

More information

Motion of Charges in Uniform E

Motion of Charges in Uniform E Motion of Charges in Unifor E and Fields Assue an ionized gas is acted upon by a unifor (but possibly tie-dependent) electric field E, and a unifor, steady agnetic field. These fields are assued to be

More information

2.003 Engineering Dynamics Problem Set 2 Solutions

2.003 Engineering Dynamics Problem Set 2 Solutions .003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study

More information

ma x = -bv x + F rod.

ma x = -bv x + F rod. Notes on Dynaical Systes Dynaics is the study of change. The priary ingredients of a dynaical syste are its state and its rule of change (also soeties called the dynaic). Dynaical systes can be continuous

More information