1 / 7

TRANSPORT PROPERTIES

TRANSPORT PROPERTIES. Ch 30. Quantity. Gradiant. Laws. Temperature. Heat. HOT. - +. Electrons. Potential. - - - - -. - - - - -. - - - - -. Mass. Pressure. -- - - - - -. - - - - - - -. - - - - - --. Mass Concentration. Momentum Velocity.

haroun
Télécharger la présentation

TRANSPORT PROPERTIES

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. TRANSPORT PROPERTIES Ch 30 Quantity Gradiant Laws Temperature Heat HOT - + Electrons Potential - - - - - - - - - - - - - - - Mass Pressure -- - - - - - - - - - - - - - - - - - -- Mass Concentration Momentum Velocity Flux = Jz = amount transported across unit area per s

  2. Flux- Gases 1 N C 6 Transport is by discrete carriers and each carrier transports a finite amount In 1 second 1/6th of all molecules present in the box of dimensions will pass through the shaded area C z # of molecules traveling along ‘Z’ = # of molecules crossing the face in one second = If each carrier transports quantity ‘q’

  3. T 2 HOT Z T 1 COLD T T1 T2 Potential Gradient in the System Z

  4. Thermal Conductivity of an Ideal Gas – Part 1 Z  Z+ C { Z  T 1 3  N C T Z -  B 1  Z 6 2 {   Z- [ ] A  T 1 3 N C T Z +   k + From ‘A’ to‘B’ = 1  Z 6 2  T 1 3 N C [ ]  Z 6 2  k From ‘C’ to ‘B’ = + [ ] - 2 =  k -  Since heat is a manifestation of K.E. and is transported via collisions between carriers, we shall consider gas collisions & mean free path ‘.’

  5. Thermal Conductivity of an Ideal Gas – Part 2 [ ] - 2  k -  Net Flux = = = = -   T  T 1 3 N C  Z  Z 6 2

  6. Mean free path ‘’  Average distance traveled in 1s = If ‘Z’, = number collisions per s, = C Consider a cylinder of radius,  , length In 1s, molecule will travel from one end to the other # collisions made by one molecule per s = But average relative velocity = A = 0 =2C =sqr2C Collision number = Mean free path = Relative Velocity

  7. Diffusion:substances diffuse from a high concentration region to a low concentration region. Z Nz+ Nz Nz- x Net Flow Homework: Poizulle Formula & Viscosimeter

More Related