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Unformatted text preview: 807 Chapter 19 1. (a) Eq. 193 yields n = M sam / M = 2.5/197 = 0.0127 mol. (b) The number of atoms is found from Eq. 192: N = nN A = (0.0127)(6.02 × 10 23 ) = 7.64 × 10 21 . 2. Each atom has a mass of m = M / N A , where M is the molar mass and N A is the Avogadro constant. The molar mass of arsenic is 74.9 g/mol or 74.9 × 10 –3 kg/mol. Therefore, 7.50 × 10 24 arsenic atoms have a total mass of (7.50 × 10 24 ) (74.9 × 10 –3 kg/mol)/(6.02 × 10 23 mol –1 ) = 0.933 kg. 3. With V = 1.0 × 10 –6 m 3 , p = 1.01 × 10 –13 Pa, and T = 293 K, the ideal gas law gives ( 29 ( 29 ( 29( 29 13 6 3 23 1.01 10 Pa 1.0 10 m 4.1 10 mole. 8.31 J/mol K 293 K pV n RT × × = = = × ⋅ Consequently, Eq. 192 yields N = nN A = 25 molecules. We can express this as a ratio (with V now written as 1 cm 3 ) N / V = 25 molecules/cm 3 . 4. (a) We solve the ideal gas law pV = nRT for n : ( 29 ( 29 ( 29( 29 6 3 8 100Pa 1.0 10 m 5.47 10 mol. 8.31J/mol K 220K pV n RT × = = = × ⋅ (b) Using Eq. 192, the number of molecules N is ( 29 ( 29 6 23 1 16 A 5.47 10 mol 6.02 10 mol 3.29 10 molecules. N nN = = × × = × 5. Since (standard) air pressure is 101 kPa, then the initial (absolute) pressure of the air is p i = 266 kPa. Setting up the gas law in ratio form (where n i = n f and thus cancels out — see Sample Problem 191), we have f f f i i i p V T pV T = CHAPTER 19 808 which yields ( 29 2 3 2 3 1.64 10 m 300K 266kPa 287 kPa 1.67 10 m 273K f i f i f i T V p p V T × = = = × . Expressed as a gauge pressure, we subtract 101 kPa and obtain 186 kPa. 6. (a) With T = 283 K, we obtain ( )( ) ( )( ) 3 3 100 10 Pa 2.50m 106mol. 8.31J/mol K 283K pV n RT ´ = = = × (b) We can use the answer to part (a) with the new values of pressure and temperature, and solve the ideal gas law for the new volume, or we could set up the gas law in ratio form as in Sample Problem 191 (where n i = n f and thus cancels out): f f f i i i p V T pV T = which yields a final volume of ( 29 3 3 100kPa 303K 2.50m 0.892 m 300kPa 283K f i f i f i T p V V p T = = = . 7. (a) In solving pV = nRT for n , we first convert the temperature to the Kelvin scale: (40.0 273.15) K 313.15 K T = + = . And we convert the volume to SI units: 1000 cm 3 = 1000 × 10 –6 m 3 . Now, according to the ideal gas law, ( 29 ( 29 ( 29( 29 5 6 3 2 1.01 10 Pa 1000 10 m 3.88 10 mol. 8.31J/mol K 313.15K pV n RT × × = = = × ⋅ (b) The ideal gas law pV = nRT leads to ( 29 ( 29 ( 29 ( 29 5 6 3 2 1.06 10 Pa 1500 10 m 493K....
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This note was uploaded on 08/09/2010 for the course PHY 202 101A2 taught by Professor Prof.yang during the Summer '10 term at National Taiwan University.
 Summer '10
 Prof.Yang
 Physics, Mass

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