Trans Pheno II Lecture 3 - Chapter 9.5-9.10

download Trans Pheno II Lecture 3 - Chapter 9.5-9.10

of 15

description

Transport Phenomena II lecture. A breif lecture.

Transcript of Trans Pheno II Lecture 3 - Chapter 9.5-9.10

  • Thermal Conductivity, k

    1

    Thermal conductivity is the property of a material that indicates its ability to conduct heat. It has unit W/mK.

    Table 9.5-1 (Gases) at 1atm pressureTable 9.5-2 (Nonmetallic Liquids) at saturation pressuresTable 9.5-3 (Liquid Metals) at atmospheric pressureTable 9.5-4 (Solids)

    k depends on temperature and pressure (same as )

  • 2Page 265

    - For rough estimation only

    - Should not be used in the neighborhood of the critical point

    - Tc, pc information in Table D.1(Page 738)

    Estimation of thermal conductivity under different T and p conditions

  • Critical Properties

    3Table not complete, see page 738

  • Example

    4

    Please estimate the thermal conductivity of methane (CH4) at 110.4 atm and 127 F.

    Express your answer with SI unit (W/mK).

  • Fundamental Mechanisms

    5

    Atomic vibrations and free electron in hotter region transport energy to cooler regions.

  • 6Thermal Conductivity: Comparisoni

    n

    c

    r

    e

    a

    s

    i

    n

    g

    k

    PolymersPolypropylene 0.12Polyethylene 0.46-0.50 Polystyrene 0.13 Teflon 0.25

    vibration/rotation of chain molecules

    CeramicsMagnesia (MgO) 38Alumina (Al2O3) 39 Soda-lime glass 1.7 Silica (cryst. SiO2) 1.4

    atomic vibrations

    MetalsAluminum 247Steel 52 Tungsten 178 Gold 315

    atomic vibrations and motion of free electrons

    k (W/m-K)Energy Transfer

    MechanismMaterial

    www.csun.edu/~bavarian/Courses/MSE%20227/Lectures_Exam3/ch17-Thermal_Properties.ppt

  • Gases k

    7

    Chapman-Enskog Formula (for monatomic gases)- Model based on rigid, nonattracting spheres of mass m

    Eucken Formula (for polyatomic gases)

    (9.7-13)

    (9.7-15)

  • 8Not complete, see Page 738-739

  • 9Not complete, see Page 740

  • Example

    10

    Estimate the thermal conductivity of Argon (Ar) at 100C and atmospheric pressure.

    Compare your result with the observed value of 506 10-7 cal/cmsK.

  • Liquids k

    11

    Bridgmans Equation: - Derived assuming monatomic liquids, but also show

    good agreement for polyatomic liquids

    (9.8-3)

    (9.8-4)

  • Example

    12

    The density of liquid CCl4 at 20 C and 1 atm is 1.595g/cm3, and its isothermal compressibility

    is

    90.710-6 atm-1. Please estimate its thermal conductivity.

  • Solids k

    13

    Usually measured experimentally due to dependence on various factors (crystallite size, degree of molecular orientation, void fraction, etc.)

    Wiedemann-Franz-Lorenz Equation:

    - ke: electrical conductivity- L: Lorenz number, 22 ~ 29 10-9 volt2/k2 at 0 C and increases

    slowly with temperature.- Only for pure metal, because free electrons are the major heat

    carriers in pure metals.

    (9.9-1)

  • Composite Solids keff

    14

    For one solid phase dispersed in a second solid phase, or solids containing pores -> effective thermal conductivity

    http://www.ruthtrumpold.id.au/designtech/pmwiki.php?n=Main.ClassifyingMaterials

    Maxwell Equation: (9.6-1)

    - Only for spherical inclusions- Assuming low volume fraction and

    uniform sphere distribution (but okay)

    See other correlations in the textbook.Find specific k information in the literature

    (9.10-1)

  • Other Important Properties

    15

    Thermal diffusivity:

    - has the same dimension as kinematic viscosity [L2/T]; - and occur in similar ways in the equations of change for momentum and energy transport

    Prandtl number:

    Peclet number: Pe = RePr

    relative ease of momentum and energy transport

    p

    kc

    Density

    Heat capacity at constant pressure

    Pr pc

    k

    rate of advection / rate of diffusion