Chemistry: The Molecular Nature of Matter, 6E Jespersen/Brady/Hyslop Group Problem In groups of 2-3 brainstorm how to describe a gas. What are some observable properties? What variables would you use to describe a gas? 2 Group Problem Describe a gas: o Will expand to fill a volume o Mostly empty space so can be compressed o Can expand & contract with temperature o Particles constantly in motion & constantly colliding o Some gases are heavier then others and sink to the floor rather then rise to the ceiling 3 Properties of Common Gases Despite wide differences in chemical properties, all gases more or less obey the same set of physical properties. Four Physical Properties of Gases Inter-related 1. Pressure (P ) 2. Volume (V ) 3. Temperature (T ) 4. Amount = moles (n) 4 Review: The Mole Avagadro’s number (NA) allows us to measure the number of particles of a gas as the number of moles: NA = 6.02214129 × 1023 particles/mole We can measure the number of moles of a gas by measuring its mass and knowing its Molar Mass Molar Mass = mass / (# of moles) M = m/n Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 5 Group Problem How many moles of the CFC pollutant CCl2F2 are in 50.0g? 6 Group Problem How many moles of the CFC pollutant CCl2F2 are in 50.0g? 50.0 g CCl2F2(1 mol/121 g CCl2F2) = 0.41 mol CCl2F2 7 Group Problem Calculate the mass of 3 moles of nerve agent VX: CH3CH2 C11H26NO2PS 8 Group Problem Calculate the mass of 3 moles of nerve agent VX: CH3CH2 3 mol C11H26NO2PS ( 267 g C11H26NO2PS /mol C11H26NO2PS) = 801 g C11H26NO2PS 9 Review: Temperature Temperature is measured with a thermometer usually in °C, °F, or Kelvin Fahrenheit O is freezing point of salt water/96 is temperature of life Celsius O is freezing point of water/100 is boiling point of water Kelvin Uses absolute 0 where all motion stops O°C = 273 K °C = (°F -32) × (5/9) 10 Group Problem If room temperature is 25°C, what is room temperature in Kelvin? In °F? 11 Group Problem If room temperature is 25°C, what is room temperature in Kelvin? RT = 25°C + 273 K = 298 K In °F? 25°C = (°F -32) × (5/9) °F = [(25°C) 9/5] +32 = 77 °F 12 Pressure: Measurement and Units force Pressure area Pressure is force per unit area Earth exerts gravitational force on everything with mass near it Weight Measure of gravitational force that earth exerts on objects with mass What we call weight is gravitational force acting on object (weight ≠ mass) 13 Force vs. Pressure Consider someone wearing flat shoes vs. high "spike" heels Weight of person is the same F = 120 lbs Pressure on floor differs greatly (F/A) Shoe Flat Spike Area Pressure 10 in. 3 in. 120 lbs P = = 4 psi 2 = 30 in.2 30 in. 0.4 in 0.4 in 120 lbs = 750 psi = 0.16 in.2 P = 2 0.16 in. This is why snow shoes have a large footprint 14 Pressure Atmospheric Pressure Resulting force per unit area When earth's gravity acts on molecules in air Pressure due to air molecules colliding with object Barometer Instrument used to measure atmospheric pressure 15 Vaccum A vacuum exerts zero pressure on a containers walls 16 Toricelli Barometer Simplest barometer Tube that is 80 cm in length Sealed at one end Filled with mercury In dish filled with mercury 17 Toricelli Barometer Air pressure Pushes down on mercury Forces mercury up tube Weight of mercury in tube Pushes down on mercury in dish When two forces balance Mercury level stabilizes Read atmospheric pressure 18 Toricelli Barometer If air pressure is high Pushes down on mercury in dish Increase in level in tube If air pressure is low Pressure on mercury in dish less than pressure from column Decrease level in tube Result: Height of mercury in tube is the atmospheric pressure 19 Standard Atmospheric Pressure Typical range of pressure for most places where people live 730 to 760 mm Hg Top of Mt. Everest Air pressure = 250 mm Hg Standard atmosphere (atm) Average pressure at sea level Pressure needed to support column of mercury 760 mm high measured at 0 °C 20 Units of Pressure SI unit for pressure Pascal = Pa = 1 N/m2 1 atm = 101,325 Pa = 101 kPa 100 kPa = 0.9868 atm Other units of pressure 1.013 Bar = 1013 mBar = 1 atm 760 mm Hg = 1 atm 760 torr = 1 atm At sea level 1 torr = 1 mm Hg 21 Group Problem Express Pressure in atm and kPa for a gas at 705 mmHg 22 Group Problem Express Pressure in atm and kPa for a gas at 705 mmHg. 705 mmHg(1 atm/760 mmHg) = 0.927 atm 0.927 atm (101 kPa/1 atm) = 93.6 kPa 23 Manometers Used to measure pressure inside closed reaction vessels Pressure changes caused by gases produced or used up during chemical reaction Open-end manometer U tube partly filled with liquid (usually mercury) One arm open to atmosphere One arm exposed to trapped gas in vessel 24 Open Ended Manometer Pgas = Patm Pgas > Patm Gas pushes mercury up tube Pgas < Patm Atmosphere pushes mercury down tube 25 Ex. Using Open Ended Manometers A student collected a gas in an apparatus connected to an openend manometer. The mercury in the column open to the air was 120 mm higher and the atmospheric pressure was measured to be 752 torr. What was the pressure of the gas in the apparatus? This is a case of Pgas > Patm Pgas = 752 torr + 120 torr = 872 torr 26 Ex. Using Open Ended Manometers In another experiment, it was found that the mercury level in the arm of the manometer attached to the container of gas was 200 mm higher than in the arm open to the air. What was the pressure of the gas? This is a case of Pgas < Patm Pgas = 752 torr – 200 torr = 552 torr 27 Group Problem CO2 collected in a monometer in a lab with a barometric reading of 97 kPa. What is the Pressure of CO2? 33 mmHg 28 Group Problem CO2 collected in a monometer in a lab with a barometric reading of 97 kPa. What is the Pressure of CO2? Pgas < Patm 33mm Hg (101 kPa/760 mmHg) =4.4 kPa Pgas = 97 kPa – 4.4 kPa = 92.06 kPa 33 mmHg 29 Closed-end Manometer Arm farthest from vessel (gas) sealed Tube filled with mercury Then open system to flask and some mercury drains out of sealed arm Vacuum exists above mercury in sealed arm 30 Closed-end Manometer Level of mercury in arm falls, as not enough pressure in the flask to hold up Hg Patm = 0 Pgas = PHg So directly read pressure 31 Your Turn Gas pressure is measured using a close-ended mercury manometer. The height of fluid in the manometer is 23.7 in. Hg. What is this pressure in atm? A. 23.7 atm B. 0.792 atm C. 602 atm D. 1.61 atm 2.54 cm 10 mm 1 atm 23.7 in. Hg ´ ´ ´ = 0.792 atm in cm 760 mm 32 Group Problem What is the pressure of an unknown gas in atm within this closed monometer? Closed monometer 437 mm 205 mm 33 Group Problem What is the pressure of an unknown gas in atm within this closed monometer? PHg = 437mm-205mm = 232mm Closed monometer 232mmHg (1 atm/160 mmHg) 437 mm = 0.31 atm 205 mm 34 Comparison of Hg and H2O Pressure of 1 mm column of mercury and 13.6 mm column of water are the same Mercury is 13.6 times more dense than water Both columns have same weight and diameter, so they exert same pressure d = 13.6 g/mL d = 1.00 g/mL 35 Using Liquids Other Than Mercury in Manometers and Barometers Simple relationship exists between two systems. For example, use water (d = 1.00 g/mL) instead of mercury (d = 13.6 g/mL) in the tube In general hA d A hB d B For converting from mm Hg to mm H2O hH O = 2 hHg ´ d Hg dH O 2 Use this relationship to convert pressure change in mm H2O to pressure change in mm Hg 36 Ex. Converting mm Acetone to mm Hg - Solution Acetone has a density of 0.791 g/mL. Acetone is used in an open-ended manometer to measure a gas pressure slightly greater than atmospheric pressure, which is 756 mm Hg at the time of the measurement. The liquid level is 20.4 mm higher in the open arm than in the arm nearest the gas sample. What is the gas pressure in torr? 37 Ex. Converting mm Acetone to mm Hg - Solution First convert mm acetone to mm Hg hHg 20.4 mm acetone ´ 0.791 g/mL = = 1.19 mm Hg 13.6 g/mL Then add PHg to Patm to get Ptotal Pgas = Patm + PHg = 756.0 torr + 1.19 torr Pgas = 757.2 torr 38 Boyle’s Law Studied relationship between P and V Work done at constant T as well as constant number of moles (n) T1 = T2 As V decreases, P increases 39 Ideal Gas Law Charles Law If Pressure is constant but freeze a balloon, it decreases in V Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 40 Charles’s Law Charles worked on relationship of how V changes with T Kept P and n constant Demonstrated V increases as T increases 41 Gay-Lussac’s Law Worked on relationship between pressure and temperature Volume (V ) and number of moles (n) are constant P increases as T increases This is why we don’t heat canned foods on a campfire without opening them Showed that gas pressure is directly proportional to absolute temperature P µT Low T, Low P P High T, High P T (K) 42 Group Problem Force of Collisions P Area What happens to gas pressure when you raise the temperature? If the container can expand in response to the force In a rigid walled container 43 Group Problem Force of Collisions P Area What happens to gas pressure when you raise the temperature? If the container can expand in response to the force No change in pressure is observed because the area increased. In a rigid walled container Pressure increases because the faster moving molecules hit the walls of the container with greater force 44 Combined Gas Law 1 o Boyle’s law: P V o Charles Law: T V o Guy-Lussac’s Law: o T P V T P is equivalent to o For any two conditions: Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E T P V PV =C T P1V1 P2V2 T1 T2 45 Combined Gas Law P1V1 P2V2 = T1 T2 All T 's must be in K Value of P and V can be any units as long as they are the same on both sides Can derive Boyle’s Law, Charle’s Law, and Guy Lussac’s Law from this equation Gives all relationships needed for fixed amount of gas under two sets of conditions 46 How Other Laws Fit into Combined Gas Law P1V1 T1 = Boyle’s Law T1 = T2 Charles’ Law P1 = P2 Gay-Lussac’s V1 = V2 Law P2V2 T2 P1V1 = P2V2 V1 T1 P1 T1 = = V2 T2 P2 T2 47 Combined Gas Law P1V1 T1 = P2V2 T2 Used for calculating effects of changing conditions T in Kelvin P and V any units, as long as units cancel Example: If a sample of air occupies 500. mL at 273.15 K and 1 atm, what is the volume at 85 °C and 560 torr? 760 torr ´ 500. mL 273.15 K = 560 torr ´ V2 358 K V2 = 890. mL 48 Ex. Using Combined Gas Law What will be the final pressure of a sample of nitrogen gas with a volume of 950. m3 at 745 torr and 25.0 °C if it is heated to 60.0 °C and given a final volume of 1150 m3? First, number of moles is constant even though actual number is not given You are given V, P and T for initial state of system as well as T and V for final state of system and must find Pfinal This is a clear case for combined gas law 49 Ex. Using Combined Gas Law List what you know and what you don’t know Convert all temperatures to Kelvin Then solve for unknown—here P2 P1 = 745 torr P2 = ? V1 = 950 m3 V2 = 1150 m3 T1 = 25.0 °C + 273.15 T2 = 60.0 °C + 273.15 = 298.15 K P2 = P1V1T2 T1V2 = = 333.15 K 745 torr ´ 950 m3 ´ 333.15 K P2 = 688 torr 3 298.15 K ´ 1150 m 50 Ex. Combined Gas Law Anesthetic gas is normally given to a patient when the room temperature is 20.0 °C and the patient's body temperature is 37.0 °C. What would this temperature change do to 1.60 L of gas if the pressure and mass stay the same? V1 T1 = What do we know? P and n are constant So combined gas law simplifies to V2 T2 51 Ex. Combined Gas Law V1 = 1.60 L V2 = ? T1 = 20.0 °C + 273.15 T2 = 37.0 °C + 273.15 = 293.15 K = 310.15 K List what you know and what you don’t know Convert all temperatures to Kelvin Then solve for unknown—here V2 V2 = V1T2 T1 1.60 L ´ 310.15 K = 293.15 K V2 = 1.69 L 52 Your Turn Which units must be used in all gas law calculations? A. K for temperature B. atm for pressure C. L for volume D. no specific units as long as they cancel 53 Relationships between Gas Volumes In reactions in which products and reactants are gases: If T and P are constant Simple relationship among volumes hydrogen + chlorine hydrogen chloride 1 vol 1 vol 2 vol hydrogen + oxygen water (gas) 2 vol 1 vol 2 vol Ratios of simple, whole numbers 54 Avogadro’s Principle When measured at same T and P, equal V 's of gas contain equal number of moles Volume of a gas is directly proportional to its number of moles, n V is proportional to n (at constant P and T ) Coefficients Volumes Molecules Moles H2(g) + Cl2(g) 2 HCl(g) 1 1 2 1 1 2 1 1 2 (Avogadro's Principle) 1 1 2 55 Standard Molar Volume Volume of 1 mole gas must be identical for all gases under same P and T Standard conditions of temperature and pressure — STP STP = 1 atm and 273.15 K (0.0 °C) Under these conditions 1 mole gas occupies V = 22.4 L 22.4 L standard molar volume 56 Learning Check: Calculate the volume of ammonia formed by the reaction of 25 L of hydrogen with excess nitrogen. N2(g) + 3H2(g) 2NH3(g) 25 L H2 2 L NH3 ´ = 17 L NH3 1 3 L H2 57 Learning Check: N2(g) + 3H2(g) 2NH3(g) If 125 L H2 react with 50 L N2, what volume of NH3 can be expected? 125 L H2 2 L NH3 ´ = 83.3 L NH3 1 3 L H2 50 L N2 2 L NH3 ´ = 100 L NH3 1 1 L N2 H2 is limiting reagent 83.3 L 58 Learning Check: How many liters of N2(g) at 1.00 atm and 25.0 °C are produced by the decomposition of 150. g of NaN3? 2NaN3(s) 2Na(s) + 3N2(g) 150. g NaN 3 1 mol NaN 3 3 mol N2 ´ ´ = 3.461 mol N2 1 65.0099 g 2 mol NaN 3 3.461 mol N2 22.4 L ´ = 77.53 L 1 1 mol at STP V 1 V2 V 1T2 = ; V2 = T 1 T2 T1 77.53 L ´ 298.15 K V2 = = 84.6 L 273.15 K 59 Your Turn How many liters of SO3 will be produced when 25 L of sulfur dioxide reacts with 75 L of oxygen ? All gases are at STP. A. 25 L B. 50 L C. 100 L D. 150 L E. 75 L 2SO2(g) + O2(g) 25 L SO2 ´ 75 L O2 ´ 2SO3(g) 2 L SO3 2 L SO2 2 L SO3 1 L O2 = 25 L SO3 = 150 L SO3 60 Ideal Gas Law With Combined Gas Law we saw that PV =C T With Avogadro’s results we see that this is modified to PV = n ´R T Where R = a new constant = Universal Gas constant PV = nRT 61 Ideal Gas Law PV = nRT Equation of state of a gas: If we know three of these variables, then we can calculate the fourth Can define state of the gas by defining three of these values Ideal Gas Hypothetical gas that obeys ideal gas law relationship over all ranges of T, V, n and P As T increases and P decreases, real gases act as ideal gases 62 What is the value of R? Plug in values of T, V, n and P for 1 mole of gas at STP (1 atm and 0.0 °C) T = 0.0 °C = 273.15 K P = 1 atm V = 22.4 L n = 1 mol PV 1 atm ´ 22.4 L R= = nT 1 mol ´ 273.15 K R = 0.082057 L atm mol–1 K–1 63 Learning Check: PV = nRT How many liters of N2(g) at 1.00 atm and 25.0 °C are produced by the decomposition of 150. g of NaN3? 2NaN3(s) 2Na(s) + 3N2(g) V=? V = nRT/P P = 1 atm T = 25C + 273.15 = 298.15 K 150. g NaN 3 1 mol NaN 3 3 mol N2 n = mol N2 = ´ ´ 1 65.01 g 2 mol NaN 3 n = 3.461 mol N2 3.461 mol N ) ( 0.082057 ( V = 2 1.00 atm L×atm mol×K ) (298.15 K ) V = 84.6 L Ex. Ideal Gas Law Problem What volume in milliliters does a sample of nitrogen with a mass of 0.245 g occupy at 21 °C and 750 torr? What do I know? Mass and identity (with the MM) of substance – can find moles Temperature Pressure What do I need to find? Volume in mL 65 Ex. Ideal Gas Law Problem Solution V = ? (mL) mass = 0.245 g MM = 2 14.0 = 28.0 g/mol Convert temperature from °C to K T = 21°C + 273.15 K = 294 K Convert pressure from torr to atm æ 1 atm ö ÷÷ =0.987 atm P = 750 torr çç è 760 torr ø Convert mass to moles m 0.245 g –3 n= = =8.75 ´ 10 mol MM 28.0 g mol–1 66 Ex. Ideal Gas Law Problem Solution nRT V = P 8.75 10 V 3 moles 0.082057 L atm mol -1 K -1 294 K 0.987 atm 1000 mL V = 0.214 L ´ = 214 mL 1L 67 Your Turn Dry ice is solid carbon dixoide. What is the pressure, in atm, of CO2 in a 50.0 L container at 35 °C when 33.0 g of dry ice becomes a gas? A. 0.043 atm B. 0.010 atm C. 0.38 atm D. 0.08 atm æ 1 mol CO ö æ ö E. 38 atm L atm 2 (33.0 g CO ) ççè 44.01 g CO ÷÷øççè0.0821 K mol ÷÷ø (308 K) 2 Pressure of CO2 = = 0.38 atm 2 50.0 L 68 Group Problem N2 + H2 NH3 How much H2 at 0°C and 0.86 atm do you need to react completely with 750 mL of N2 at 1.5 atm and 20°C to form ammonia? Hint: is this equation balanced? 69 Group Problem N2 + 3 H2 2 NH3 How much H2 at 0°C and 0.86 atm do you need to react completely with 750 mL of N2 at 1.5 atm and 20°C to form ammonia? nN2 = PV/RT = (1.5 atm)(0.750L)/[(0.082 L atm mol–1 K–1)(293K)]= 0.047 mol 0.047 mol Nz (3 mol Hz/1 molN2) = 0.14 mol H2 V = nRT/P = [(0.14 mol)(0.082 L atm mol–1 K–1)(273K)]/0.86 atm = 3.66L H2 Or another way: 750 mL N2 *(3 mL H2/1 mLN2) = 2250 mL H2 - at 1.5 atm and 20 °C (1.5 atm)(2250 mL)/293 K = 0.86 atm(VH2)/273 VH2 = 3656 mL = 3.6 L 70 Group Problem A sample of helium gas occupies 500.0 mL at 1.21 atm Calculate the volume of the gas if the pressure is reduced to 491 torr Group Problem A sample of helium gas occupies 500.0 mL at 1.21 atm Calculate the volume of the gas if the pressure is reduced to 491 torr Use Boyle’s Law: P1V1 = P2V2 1.21 atm(500.0 mL) = 491 torr(1atm/760 torr)(V2) V2 = 936.5 mL Determining Molecular Mass of Gas If you know P, T, V and mass of gas Use ideal gas law to determine moles (n) of gas Then use mass and moles to get MM If you know T, P, and density (d ) of a gas Use density to calculate volume and mass of gas Use ideal gas law to determine moles (n) of gas Then use mass and moles to get MM 73 Ex. Molecular Mass of a Gas The label on a cylinder of an inert gas became illegible, so a student allowed some of the gas to flow into a 300 mL gas bulb until the pressure was 685 torr. The sample now weighed 1.45 g; its temperature was 27.0 °C. What is the molecular mass of this gas? Which of the Group 7A gases (inert gases) was it? What do I know? V, mass, T and P 74 Ex. Molar Mass of a Gas 1L = 0.300 L V = 300 mL ´ 1000 mL Mass = 1.45 g Convert T from °C to K T = 27.0 °C + 273.15 K = 300.2 K Convert P from torr to atm 1 atm P = 685 torr ´ = 0.901 atm 760 torr Use V, P, and T to calculate n ( )( ) )( 0.901 atm 0.300 L PV n= = = 0.01098 RT 0.082057 atm L mol–1 K –1 300.2 K mole 75 ( ) Ex. Molar Mass of a Gas – Solution Now use the mass of the sample and the moles of the gas (n) to calculate the molar mass (MM) Molar Mass = mass n 1.45 g = = 132 g/mol 0.01098 mol Gas = Xe (Atomic Mass = 131.29 g/mol) 76 Ex. Molecular Mass and Molecular Formula of a Gas A gaseous compound of phosphorus and fluorine with an empirical formula of PF2 was found to have a density of 5.60 g/L at 23.0 °C and 750 torr. Calculate its molecular mass and its molecular formula. Know Density Temperature Pressure 77 Ex. Molecular Mass and Molecular Formula Solution 1 L weighs 5.60 g So assume you have 1 L of gas V = 1.000 L Mass = 5.60 g Convert T from °C to K T = 23.0 °C + 273.15 K = 296.2 K Convert P from torr to atm d = 5.60 g/L 1 atm P = 750 torr ´ = 0.9868 atm 760 torr 78 Ex. Molecular Mass and Molecular Formula Solution ( )( ) 0.9868 atm 1.000 L PV n= = = RT 0.082057 L atm mol–1 K –1 296.2 K ( )( ) 0.04058 mole Use n and mass to calculate molar mass Molar Mass = mass n 5.60 g = = 138 g/mol 0.04058 mol 79 Ex. Molecular Mass and Molecular Formula Solution Now to find molecular formula given empirical formula and MM First find mass of empirical formula unit 1 P = 1 31 g/mol = 31 g/mol 2 F = 2 19 g/mol = 38 g/mol Mass of PF2 = 69 g/mol molecular mass 138 g/mol = =2 empirical mass 69 g/mol The correct molecular formula is P2F4 80 Which Gas Law to Use? Which gas law to use in calculations? If you know ideal gas law, you can get all the rest Amount of gas given or asked for in moles or g Use Ideal Gas Law PV = nRT Amount of gas remains constant or not mentioned Gas Law Problems Use Combined Gas Law P1V1 P2V2 = n1T1 n2T2 81 Your Turn A 7.52 g sample of a gas with an empirical formula of NO2 occupies 2.0 L at a pressure of 1.0 atm and 25 °C. Determine the molar mass and molecular formula of the compound. A. 45.0 g/mol, NO2 B. 90.0 g/mol, N2O4 C. 7.72 g/mol, NO D. 0.0109 g/mol, N2O E. Not enough data to determine molar mass 82 Your Turn - Solution Molar Mass = g/mol Know mass = 7.52 g Moles = n= PV/RT Therefore MM = 7.52g /[PV/RT] = 7.52g * (RT/PV) 7.52 g) ( 0.0821 L atm K mol ) (298 K ) ( Molar Mass = (1.0 atm) (2.0 L ) –1 –1 92.0 g/mol = 90.0 æ 90 92 g mol–1 ö çç ÷ =2 –1 ÷ è 45.0 46 g mol ø Molecular formula is N2O 4 83 Stoichiometry of Reactions Between Gases Can use stoichiometric coefficients in equations to relate volumes of gases Provided T and P are constant Volume is proportional to moles (V n) 84 Ex. Stoichiometry of Gases Methane burns with the following equation: CH4(g) + 2O2(g) CO2(g) + 2H2O(g) 1 vol 2 vol 1 vol 2 vol The combustion of 4.50 L of CH4 consumes how many liters of O2? (Both volumes measured at STP.) P and T are all constant so just look at ratio of stoichiometric coefficients Volume of O2= 4.50 L ´ = 9.00 L O2 2 L O2 1 L CH4 85 Ex. Ideal Gas Law In one lab, the gas collecting apparatus used a gas bulb with a volume of 250 mL. How many grams of Na2CO3(s) would be needed to prepare enough CO2(g) to fill this bulb when the pressure is at 738 torr and the temperature is 23 °C? The equation is: Na2CO3(s) + 2 HCl(aq) 2 NaCl(aq) + CO2(g) + H2O 86 Ex. Ideal Gas Law – Solution What do I know? T, P, V and MM of Na2CO3 What do I need to find? Mass of Na2CO3 How do I find this? Use ideal gas law to calculate moles CO2 Convert moles CO2 to moles Na2CO3 Convert moles Na2CO3 to grams Na2CO3 87 Ex. Ideal Gas Law – Solution 1. Use ideal gas law to calculate moles CO2 a. First convert mL to L 1L V = 250 mL ´ = 0.250 L 1000 mL a. Convert torr to atm 1 atm P = 738 torr ´ = 0.971 atm 760 torr b. Convert °C to K T = 23.0 °C + 273.15 K = 296.2 K 88 Ex. Ideal Gas Law – Solution 1. Use ideal gas law to calculate moles CO2 PV 0.971 atm ´ 0.250 L n= = RT 0.082057 atm L mol–1 K –1 ´ 296.2 K = 9.989 × 10–3 mole CO2 2. Convert moles CO2 to moles Na2CO3 1 mol Na 2 CO3 9.989 10 mol CO 2 1 mol CO 2 –3 = 9.989 × 10–3 mol Na2CO3 89 Ex. Ideal Gas Law – Solution 3. Convert moles Na2CO3 to grams Na2CO3 9.989 ´ 10-3 æ 106 g Na CO ö 2 3÷ mol Na2CO3 çç ÷ 1 mol Na CO è 2 3 ø = 1.06 g Na2CO3 90 Your Turn 2Na(s) + 2H2O(l ) → 2NaOH(aq) + H2(g) How many grams of sodium are required to produce 20.0 L of hydrogen gas at 25.0 °C, and 750 torr? A. 18.6 g B. 57.0 g C. 61.3 g D. 9.62 g E. 37.1 g 91 Your Turn - Solution Moles of H2 produced: n= æ 1 atm ö 750 torr çç ÷÷ 20.0 L è 760 torr ø ( ( )( ) 0.0821 L atm K –1 mol–1 298 K ) = 0.807 mol H2 Grams of sodium required: æ 2 mol Na ö æ 23.0 g ö ÷ çç ÷÷ = 37.1 g mass Na = 0.807 mol H2 çç ÷ è 1 mol H2 ø è 1 mol Na ø 92 Group Problem At what temperature will 1.50 moles of CH4 occupy a 1 L container at 10 atm? 93 Group Problem At what temperature will 1.50 moles of CH4 occupy a 1 L container at 10 atm? T= PV/nR = (10 atm)(1L) (1.50 mol)(0.082 L atm mol–1 K–1) = 81.3 K 94 Group Problem o PV = nRT od = m / V oM = m / n Write out the ideal gas law in terms of density & then in terms of molar mass 95 Ideal Gas Law Considering Density & Molar Mass o PV = nRT od=m/V oM=m/n P (m / d) = nRT d = Pm/nRT PV = (m / M) RT M = mRT/PV M / d = RT / P Jesperson, Brady, Hyslop. Chemistry: The Molecular Nature of Matter, 6E 96 Dalton's Law of Partial Pressure For mixture of non-reacting gases in container Total pressure exerted is sum of the individual partial pressures that each gas would exert alone Ptotal = Pa + Pb + Pc + ··· Where Pa, Pb, and Pc are the partial pressures Partial pressure Pressure that particular gas would exert if it were alone in container 97 Dalton’s Law of Partial Pressures Assuming each gas behaves ideally Partial pressure of each gas can be calculated from ideal gas law Pa = naRT Pb = V nbRT Pc = V So total pressure is ncRT V Ptotal = Pa + Pb + Pc + × × × = naRT V + nbRT V + ncRT V +××× 98 Dalton’s Law of Partial Pressures Rearranging Ptotal æ RT = na + nb + nc + × × × çç èV Ptotal æ RT = ntotal çç èV Or ( ) ö ÷÷ ø ö ÷÷ ø Where ntotal = na + nb + nc + ··· ntotal = sum of number moles of various gases in mixture 99 Dalton’s Law of Partial Pressures Means for mixture of ideal gases Total number of moles of particles is important Not composition or identity of involved particles Pressure exerted by ideal gas not affected by identity of gas particles Reveals two important facts about ideal gases 1. Volume of individual gas particles must be important 2. Forces among particles must not be important If they were important, P would be dependent on identity of gas 100 Ex. Partial Pressure Mixtures of helium and oxygen are used in scuba diving tanks to help prevent “the bends.” For a particular dive, 46 L He at 25 °C and 1.0 atm and 12 L O2 at 25 °C and 1.0 atm were pumped into a tank with a volume of 5.0 L. Calculate the partial pressure of each gas and the total pressure in the tank at 25 °C. 101 Ex. Partial Pressure – Solution Have two sets of conditions Before and after being put into the tank He O2 Pi = 1.0 atm Pf = PHe Pi = 1.0 atm Pf = PO2 Vi = 46 L Vi = 12 L Vf = 5.0 L Vf = 5.0 L 102 Ex. Partial Pressure – Solution First calculate pressure of each gas in 5 L tank (Pf ) using combined gas law PiVi 1 atm ´ 46 L PHe = = = 9.2 atm Vf 5L PiVi 1 atm ´ 12 L PO = = = 2.4 atm 2 Vf 5L Then use these partial pressures to calculate total pressure Ptotal = PHe + PO = 9.2 atm + 2.4 atm = 11.6 atm 2 103 Your Turn A mixture of 250 mL of methane, CH4, at 35 ˚C and 0.55 atm and 750 mL of propane, C3H8, at 35˚ C and 1.5 atm, were introduced into a 10.0 L container. What is the final pressure, in torr, of the mixture? A. 95.6 torr B. 6.20 × 104 torr C. 3.4 × 103 torr D. 760 torr E. 59.8 torr 104 Your Turn - Solution (0.55 atm) (0.250 L) PCH = 4 PC H = 3 8 10.0 L 1.5 atm 0.750 L ( )( 10.0 L ) = 0.0138 atm = 0.112 atm æ 760 torr ö ÷÷ = 95.6 torr PT = 0.0138 atm + 0.112 atm çç è atm ø ( ) 105 Mole Fractions and Mole Percents Mole Fraction (χ) Ratio of number moles of given component in mixture to total number moles in mixture cA = nA n A + nB + nC + × × × + nZ = nA n total Mole Percent (mol%) Mole % = c A ´ 100% 106 Mole Fractions of Gases from Partial Pressures æV n A = PA çç è RT If V and T are constant then, ö ÷÷ ø = constant For mixture of gases in one container æV ö PA çç ÷÷ è RT ø XA = æV ö æV ö æV PA çç ÷÷ + PB çç ÷÷ + PC çç è RT ø è RT ø è RT V RT ö æV ÷÷ + × × × + PZ çç ø è RT ö ÷÷ ø 107 Mole Fractions of Gases from Partial Pressures V cancels, leaving RT PA cA = PA + PB + PC + × × × + PZ or cA = PA Ptotal = nA n total 108 Ex. Partial Pressures The partial pressure of oxygen was observed to be 156 torr in air with a total atmospheric pressure of 743 torr. Calculate the mole fraction of O2 present Use cA = c O2 PA Ptotal 156 torr = = 0.210 743 torr 109 Partial Pressures and Mole Fractions Partial pressure of particular component of gaseous mixture Equals mole fraction of that component times total pressure PA = c A ´ Ptotal 110 Ex. Partial Pressure The mole fraction of nitrogen in the air is 0.7808. Calculate the partial pressure of N2 in air when the atmospheric pressure is 760. torr. PN =cN ´ Ptotal 2 2 PN = 0.7808 ´ 760 torr = 593 torr 2 111 Your Turn A mixture of 250 mL of methane, CH4, at 35˚ C and 0.55 atm and 750 mL of propane, C3H8, at 35˚ C and 1.5 atm was introduced into a 10.0 L container. What is the mole fraction of methane in the mixture? A. 0.50 B. 0.11 C. 0.89 D. 0.25 E. 0.33 112 Your Turn - Solution 0.55 atm ´ 0.250 L PCH4 = = 0.0138 atm 10.0 L 1.5 atm ´ 0.750 L PC 3H8 = = 0.112 atm 10.0 L 0.0138 atm c CH = = 0.110 4 0.0138 atm + 0.112 atm 113 Group Problem A mixture of 4.00 g of hydrogen and 10.0 g of helium are in a 4.30-L flask at 0°C. What is the total pressure of the container and the partial pressures of each gas? 114 Group Problem A mixture of 4.00 g of hydrogen and 10.0 g of helium are in a 4.30-L flask at 0°C. What is the total pressure of the container and the partial pressures of each gas? mol H2 = 4.00 g (1 mol H2/2.00 g H2)= 2.00 mol mol He = 10.0 g He (1 mol He/4.00 g He) = 2.50 mol Total mol = 2.00 + 2.50 = 4.50 mol P total = nRT = (4.50 mol)(0.0821 L atm/(mol K))(273 K ) = 23.5 atm V 4.30 L XH2 = 2.00 mol = 0.444 4.5 mol XHe = 2.5 mol = 0.556 4.5 mol PH2 = XH2 Ptotal = (0.444)(23.5 atm) = 10.4 atm PHe= XHe Ptotal = (0.556)(23.5 atm) = 13.1 atm 115 Collecting Gases over Water Application of Dalton’s Law of Partial Pressures Gases that don’t react with water can be trapped over water Whenever gas is collected by displacement of water, mixture of gases results Gas in bottle is mixture of water vapor and gas being collected 116 Collecting Gases over Water Water vapor is present because molecules of water escape from surface of liquid and collect in space above liquid Molecules of water return to liquid When rate of escape = rate of return Number of water molecules in vapor state remains constant Gas saturated with water vapor = “Wet” gas 117 Vapor Pressure Pressure exerted by vapor present in space above any liquid Constant at constant T When wet gas collected over water, we usually want to know how much “dry” gas this corresponds to Ptotal = Pgas + Pwater Rearranging Pgas = Ptotal – Pwater 118 Ex. Collecting Gas over Water A sample of oxygen is collected over water at 20.0 ˚ C and a pressure of 738 torr. Its volume is 310 mL. The vapor pressure of water at 20 ˚ C is 17.54 torr. a. What is the partial pressure of O2? b. What would the volume be when dry at STP? a. PO2 = Ptotal – Pwater = 738 torr – 17.5 torr = 720 torr 119 Ex. Collecting Gas – (Soln.) b. Use the combined gas law to calculate PO2 at STP P1 = 720 torr P2 = 760 torr V1 = 310 mL V2 = ? T1 = 20.0 + 273.12 = 293 K T2 = 0.0 + 273 K = 273 K P1V1 P2V 2 T1 T2 P1V1T 2 V2 T1P2 720 torr ) (310 mL ) (273 K ) ( V= (293 K ) (760 torr) 2 V2 = 274 mL 120 Your Turn An unknown gas was collected by water displacement. The following data was recorded: T = 27.0 °C; P = 750 torr; V = 37.5 mL; Gas mass = 0.0873 g; PH2O(vap) = 26.98 torr Determine the molecular weight of the gas. A. 5.42 g/mol B. 30.2 g/mol C. 60.3 g/mol D. 58.1 g/mol E. 5.81 g/mol 121 Your Turn - Solution n= PV/RT MM = g/n = g (RT/PV) gRT Molar Mass = = PV ( )( )( 0.0873 g 0.0821 L atm K –1 mol–1 300 K (750 torr - 26.98 torr) (0.0375 L) = 60.3 g/mol 122 ) Group Problem 32.5 mL of Hydrogen gas is collected over water at 25 ºC and 755 torr. What is the pressure of dry hydrogen gas? (VP25ºC = 23.76 mmHg) 123 Group Problem 32.5 mL of Hydrogen gas is collected over water at 25 ºC and 755 torr. What is the pressure of dry hydrogen gas? (VP25ºC = 23.76 mmHg) Correct Pt to find the Pdry gas: 755 torr - 23.76 torr = 731.24 torr 731 torr = Phydrogen 124 Diffusion Complete spreading out and intermingling of molecules of one gas into and among those of another gas e.g. Perfume in room 125 Effusion Movement of gas molecules Through extremely small opening into vacuum Vacuum No other gases present in other half 126 Graham's Law of Effusion Studied relationship between effusion rates and molecular masses for series of gases Rates of effusion of gases are inversely proportional to square roots of their densities, d, when compared at identical pressures and temperatures Effusion Rate 1 d Effusion Rate d k (constant P and T ) (constant P and T ) k is virtually identical for all gases Effusion Rate (A) d A Effusion Rate (B) d B k 127 Graham's Law of Effusion Rearranging dB Effusion Rate ( A ) dB Effusion Rate (B ) dA dA Finally, dA MM (constant V and n) Effusion Rate (A) dB MB Effusion Rate (B ) dA MA Result: Rate of effusion is inversely proportional to molecular mass of gas Effusion Rate MM k (constant P and T ) 128 Graham's Law of Effusion Effusion Rate MM k Heavier gases effuse more slowly Lighter gases effuse more rapidly Ex. Effusion Calculate the ratio of the effusion rates of hydrogen gas (H2) and uranium hexafluoride (UF6) - a gas used in the enrichment process to produce fuel for nuclear reactors. 129 Ex. Effusion First must compute MM's MM (H2) = 2.016 g/mol MM (UF6) = 352.02 g/mol M UF6 Effusion Rate (H2 ) Effusion Rate (UF6 ) MH2 352.02 13.2 2.016 Thus the very light H2 molecules effuse ~13 times as fast as the massive UF6 molecules. 130 Ex. Effusion For the series of gases He, Ne, Ar, H2, and O2 what is the order of increasing rate of effusion? Substance He Ne Ar H2 O2 MM 20 40 2 32 4 Lightest are fastest So H2 > He > Ne > O2 >Ar 131 Kinetic Theory and Gas Laws So far, considered gases from experimental point of view At P < 1 atm, most gases approach ideal Ideal gas law predicts behavior Does not explain it Recall scientific method Law is generalization of many observations Laws allow us to predict behavior Do not explain why 132 Kinetic Theory and the Gas Law To answer WHY it happens—must construct theory or model Models consist of speculations about what individual atoms or molecules might be doing to cause observed behavior of macroscopic system (large number of atoms/molecules) For model to be successful: Must explain observed behavior in question Predict correctly results of future experiments 133 Kinetic Theory and the Gas Laws Theories can never be proved absolutely true Often valid within defined boundaries Approximation by its very nature Bound to fail at some point One example is kinetic theory of gases Attempts to explain properties of ideal gases. Describes behavior of individual gas particles 134 Postulates of Kinetic Theory of Gases ① Gas particles are tiny, their V is negligible. ② Particles travel in a straight line, in random directions. ③ 0 intermolecular attraction. ④ Elastic collisions, no Energy is lost. ⑤ If KE α T, then assume average KE α T. 135 Postulates of Kinetic Theory of Gases A gas consists of an extremely large umber of very tiny particles that are in constant, random motion. The gas particles themselves occupy a net volume so small in relation to the volume of their container that their contribution to the total volume can be ignored. The particles often collide in perfectly elastic collisions with themselves and with the walls of the container, and they move in straight lines between collisions. 136 Real Gases Don’t conform to these assumptions Have finite volumes Do exert forces on each other However, kinetic theory of gases does explain ideal gas behavior True test of model is how well its predictions fit experimental observations 137 Kinetic Theory of Gases Explains observations Boyle’s Law Gay-Lussac’s Law Charles’ Law Avogadro's principle Dalton’s Law of Partial Pressures Graham’s Las of Effusion Absolute Zero 138 Real Gases: Deviations from Ideal Gas Law Combined Gas Law Ideal Gas Law PV = constant T PV =R nT Real gases deviate Why? 139 Real Gases Deviate from Ideal Gas Law Gas molecules do experience weak attractions 1. Don’t travel in straight lines At low T and as P increases this causes problems Gas molecules have finite volumes 2. They take up space At high P this causes problems 140 Real Gases 2. Particles do attract each other Even weak attractions means they hit walls of container less often Therefore, pressure is less than ideal gas 141 Effect of Attractive Forces on Real Gas 142 van der Waal's equation for Real Gases 2 ö æ na ççP + ÷÷ V - nb = nRT 2 V ø è ( corrected P ) corrected V a and b are van der Waal's constants Obtained by measuring P, V, and T for real gases over wide range of conditions 143 van der Waal's equation for Real Gases n 2a P 2 V nb nRT V corrected P a — Pressure correction Indicates some attractions between molecules Large a Means strong attractive forces between molecules Small a Means weak attractive forces between molecules 144 van der Waal's equation for Real Gases 2 ö æ na ççP + ÷÷ V - nb = nRT 2 V ø è ( ) corrected V b — Volume correction Deals with sizes of molecules Large b Means large molecules Small b Means small molecules Gases that are most easily liquefied have largest van der Waal's constants 145 Earth’s atmosphere Layers of gases 75% of mass below 11 km 99% of mass below 30 km Air 78.08% N2 20.95% O2 0.93 % Ar 0.04 % trace gases CO2 up to 0.038% of trace H2O vapor 0-4% 146 Mono or diatomic? Think about valence electrons and reactivity of each element If an element has a full valence electron shell then it will not be very reactive Nobel gases (He, Ne, Ar, Kr, Xe, Rn) If an element has an incomplete valence electron shell it will be reactive and can even bond to itself as long as bonding rules are followed Br2, I2, N2, Cl2, H2, O2, F2 147