chap3.pdf

Upload: arisnurhidayat

Post on 06-Jan-2016

214 views

Category:

Documents


1 download

TRANSCRIPT

  • Exercises

    3.8 (a) The internal energy of a perfect monatomic gas relative to its value at T = 0 is . 32nRT

    Calculate and for the gas.UV

    T HV

    T

    Atkins says, that (3). The question gives us . dUUV

    dVUT

    dTT V= +

    U nRT=

    32

    Holding T constant and rearranging this gives us . Since T is held

    UV V

    nRTT T =

    32

    constant, the right side of the equation becomes 0. UV

    T = 0

    The definition of enthalpy is . Replacing p with its Gas Law equivalent and H U pV= +taking the partial derivative with respect to V leaves us with the equation

    . It has already been said that , and

    HV

    UV

    nRTV

    T T T =

    +

    UV

    T

    = 0

    because T is held constant. That leaves .nRTV

    T = 0HV

    T = 0

    Problems3.23 The speed of sound, , in a gas of molar mass M is related to the ratio of the heatcs

    capacities by . Show that , where is the mass ( )c RT Ms = / /1 2 ( )c ps = / /1 2 density of the gas. Calculate the speed of sound in argon at 25 degrees C.

    Rearranging the Gas Law for M gives us , and inserting this into the equation givenMRTp

    =

    gives us .cp

    s =

    1 2/

  • Variables

    5/3R due to the fact that argon is monatomicR 8.31451 jk-1mol-1

    M 39.95*10-3 Kgmol-1

    T 298.5 K

    Inserting this data into the equation , gives us the value 322 ms-1. This value( )c RT Ms = / /1 2is somewhat slower than the speed of sound in air, which is to be expected due to the increasedmolar mass of argon.