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UT CH 301 - Unit1Day6-VandenBout

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Unit1Day6 VandenBout Monday September 16 2013 3 53 PM Vanden Bout LaBrake Crawford CH301 GAS WRAP Day 6 CH301 Vanden Bout LaBrake Spring 2013 Important Information EXAM REVIEW EXAM ROOMS VANDEN BOUT 9 30 section 52130 BUR 106 version numbers 1 250 WELCH 3 502 versions numbers 251 CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 1 QUIZ CLICKER QUESTION 1 points for CORRECT answer Which of the following relationships is a supported by Dalton s Law of Partial Pressure A B C D E PV nRT P V nb nRT Ptotal XiPi Pi XiPtotal Pi XtotalPtotal CH301 Vanden Bout LaBrake Fall 2013 QUIZ CLICKER QUESTION 2 points for CORRECT answer Non Ideal Gas behavior can be modeled empirically by accounting for the non ideal behavior with correction terms The Hard Sphere model corrects for the fact that the space that the molecules occupy matters and thus the measured volume is no longer the volume that is available to the gas particles in a particular sample A TRUE B FALSE CH301 Vanden Bout LaBrake Fall 2013 WHAT DO YOU THINK When working on an in class learning activity if I get stuck then I typically A Give up and wait for the answer to be given Unit1Day6 VandenBout Page 2 When working on an in class learning activity if I get stuck then I typically A B C D Give up and wait for the answer to be given Ask classmate sitting by me a question Raise my hand so I can ask one of the TAs for help Go back over what I did in order to figure out where I went wrong E Not Applicable for I have not gotten stuck yet CH 301 Vanden Bout LaBrake Spring 2013 Jimmy Neuroscience Major http www youtube com watch v hQU6TuBkXUk feature youtu be CH 301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 3 WHAT should YOU do when you are STUCK Face the Challenge Willing to engage in the learning opportunities in each class Exert Effort Willing to work hard and practice in pursuit of understanding Seek Help Willing to ask for help when you are stuck Ambrose et al 2010 CH 301 Vanden Bout LaBrake Fall 2013 What are we going to learn today Understand Gas Behavior 1 Empirical Model Gas Laws Density number and mass Molar Mass Gas Stoichiometry Mixtures Physical Model Kinetic Molecular Gas velocity distribution Diffusion and Effusion Limits of Models Assumptions Correction Factors CH302 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 4 DEMONSTRATE SOME GAS BEHAVIORS Demonstrate Volume varying with pressure Empirical Model 1660 ish Boyle Demonstrate Volume varying with temperature Empirical Model 1780 ish Charles Demonstrate Pressure varying with amount of gas Empirical model 1810 ish Avogadro CH301 Vanden Bout LaBrake Fall 2013 Combining the Laws PV nRT The empirically derived laws are very useful in solving 2 STATE PROBLEMS 1 STATE PROBLEMS CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 5 QUIZ CLICKER QUESTION 1 A 5 0 mol sample of Ne is confined in a 3 14 L vessel at a pressure of 2 5 atm What is the number density of the gas What is the mass density of the gas A B C D Not enough information 1 6 mol L 32 g L 32 mol L 1 6 g L 16 mol L 3 2 g L CH301 Vanden Bout LaBrake Fall 2013 QUIZ CLICKER QUESTION 2 What is the total pressure of the gas mixture that contains 0 267 atm He 0 317 atm Ar 0 277 atm Ne http ch301 cm utexas edu simulations gas laws GasLawSimulator swf CH301 Vanden Bout LaBrake Fall 2013 QUIZ CLICKER QUESTION 3 What is the mole fraction of Ar in a gas mixture that contains 0 267 atm He 0 317 atm Ar 0 277 atm Ne Unit1Day6 VandenBout Page 6 What is the mole fraction of Ar in a gas mixture that contains 0 267 atm He 0 317 atm Ar 0 277 atm Ne CH301 Vanden Bout LaBrake Fall 2013 Physical Model KMT The next three questions are to be discussed amongst the sectors and answers are to be put on paper Everyone should try to get something on paper first then share results and pick the best A representative will come to document camera to share results Bragging rights are on the line CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 7 Physical Model I KMT MARSHMALLOW IN SYRINGE FULL EXPLANATION BOTH MACROSCOPIC PROPERTIES AND MICROSCOPIC MODELING CH301 Vanden Bout LaBrake Fall 2013 Physical Model II KMT BALLOON DIPPED IN LIQUID NITROGEN PROVIDE A FULL MACROSCOPIC AND MICROSCOPIC DESCRIPTION CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 8 Physical Model III KMT BALLOON IN VACUUM CHAMBER PROVIDE A FULL MACROSCOPIC AND MICROSCOPIC DESCRIPTION OF GAS CH301 Vanden Bout LaBrake Fall 2013 QUIZ CLICKER QUESTION 4 You have two gases under identical conditions One gas has a density that is double that of the other gas What is the ratio of the rate of diffusion of the high density gas compared lower density gas A B C D E 2 times less Sqrt 2 times less 2 times faster sqrt 2 times faster they are identical CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 9 QUIZ CLICKER QUESTION Given the following reaction 2CO O2 2CO2 Initially you have a container with 2 moles of CO gas and 3 moles of O2 gas at a constant temperature of 25 C and a constant pressure of 1 atm What is the final volume after the reaction is complete What is the partial pressure of the CO2 gas CH301 Vanden Bout LaBrake Fall 2013 The IGL can be derived mathematically given the following assumptions assumptions of the KMT The particles are so small compared with the distance between them that the volume of the individual particles can be assumed to be negligible zero The particles are in constant motion The collisions of the particles with the walls of the container are the cause of the pressure exerted by the gas The particles are assumed to exert no forces on each other they are assumed to neither attract nor repel each other The average kinetic energy of a collection of gas particles is assumed to be directly proportional to the Kelvin temperature of the gas CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 10 Upon conditions when the gases do not follow those assumptions must correct the model Examples Hard Sphere Model and Vander Waal s Model CH301 Vanden Bout LaBrake Fall 2013 Unit1Day6 VandenBout Page 11


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