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复旦大学:《大学物理——热学》课程教学资源(PPT课件)第10次课

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大学物理(热学) 1) Mean Free Path 2)Diffusion, Thermal conductivity, and viscosity 2006-10-12

大学物理(热学) 1) Mean Free Path 2) Diffusion, Thermal conductivity, and Viscosity 2006-10-12

Equilibrium distribution v2n1n2+n22+ ∑(舞)一 n -the number of molecules of dn is the number of molecules in vx>vx+dvx near v V,→V,+dv ν→)1+dv

Equilibrium distribution N v v v v N 2 2 2 2 2 1 + + + =  dn is the number of molecules x x x v →v + dv vy vy + dv → y z z z v → v + dv in   →        =   N n v N n v i i i 2 2 d N n v  + n v  + = 2 2 2 2 1 1 ni ⎯ the number of molecules of i v  near v

Meaning of dn/n among N molecules, how many are near probability that one molecule is near v proportional to avx fly dv dn(vr,vy,v =/()如yv,y,fvk N

among N molecules, how many are near v probability that one molecule is near v proportional to dvx ... ( ) x x f v dv Meaning of dn/N ( )d ( )d ( )d d ( , , ) x x y y z z x y z f v v f v v f v v N n v v v =  

Isotropic assumption (v,/(v,)(2)=m2)=V2+y+n2) The solution is (v,)=Cexp(2/a2) The probability should be normalized dn

Isotropic assumption ( ) ( ) ( ) ( ) ( ) 2 2 2 2 x y z x y z f v f v f v = v = v + v + v ( ) ( ) 2 2 f vx =Cexp − vx  The solution is The probability should be normalized   = N dn 1

∫=c=/) 2/a2 1=Cl explvx ly each normalized √兀 a exp C C

 ( )  3 3 2 2 exp d d 1   = −  = x x C v v N n             − =  − x x v v C exp d 1 2 2  ( )  = − x x 1 C exp v dv 2 2  12    =  1 each normalized

dn( +13+12 d v. av. av a√r exp 3k T Known v C dn(vr, vy, v)3 whule C N 2

( ) exp d d d 1 d ( , , ) 2 2 2 2 3 x y z x y z x y z v v v v v v N n v v v         + + −          =    = ? m k T v 3 2 B Known = 2 2 2 2 d ( , , ) 3  =    = N n v v v v v while x y z

dr mlv+.+ exp d v..av 2R B 2KT For unit volume dnlvx,y7 m(2+n2+2) =no 2kBT expI d v dv.av ckpT Maxwell velocity distribution

( ) ( ) x y z x y z x y z v v v k T m v v v k T m N n v v v d d d 2 exp 2 d , , B 3 2 2 2 2 B         + + −          = For unit volume d ( , , ) x y z n v v v Maxwell velocity distribution ( ) x y z x y z v v v k T m v v v k T m n d d d 2 exp 2 B 3 2 2 2 2 B 0         + + −          =

dn(v) exp 4πv2dv 2TRB nof(v)vdv Maxwell speed distribution Most probable speed For one molecule, what speed is most possible? Among N molecules, what is the speed most molecules have in unit interval?

v v k T m v k T m n v n 4 d 2 1 exp 2 d ( ) 2 B 2 3 2 B 0              −          = Maxwell speed distribution For one molecule, what speed is most possible? Most probable speed n f (v)4 v dv 2  0  Among N molecules, what is the speed most molecules have in unit interval?

dy exp-2 kBT 0 dy kOt Maxwellian can be written as 3/2 n(v 4 2 exp d m

0 2 1 exp d d B 2 2 =                 − k T mv v v m k T v B m 2 = v v v v N v n v exp d 1 4 d ( ) 2 2 m 2 3 2 2 m         −          =  Maxwellian can be written as

The average speed v=4 vexp(-v2/1mh2dv 0 m 8kT 几1

The average speed v ( v v )v v v v exp d 1 4 2 2 m 2 0 3 2 2 m −          =    m k T  = 8 B v x x x e d 4 2 0 3 m −    =

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