Download Diffusion Processes During Drying of Solids by K. N. Shukla PDF
By K. N. Shukla
The propagation of three-d surprise waves and their mirrored image from curved partitions is the topic of this quantity. it really is divided into components. the 1st half offers a ray procedure. this is often in response to the growth of fluid houses in strength sequence at an arbitrary aspect at the surprise entrance. non-stop fractions are used. effects for surprise propagation in non-uniform fluids are given. the second one half discusses the surprise mirrored image from a concave physique. the real shock-focusing challenge is integrated. The paintings is supported via either numerical and experimental effects. Many positive aspects, similar to formation of a jet, vortices and the looks of disturbances at the surprise entrance, are mentioned. in addition to surprise waves in gases, the unique positive aspects of outrage propagation via a weakly ionized plasma are thought of
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Int. 257-66. Technik" 2nd ed ( S p r i n g e r , Krischer, 0 . , 1963). VDI Forschungscheft (Dusseldorf 1959) 437. 25. , I n t . 3. Heat Mass T r a n s f e r 26. 3. Narang, 27. 28. and (1965) 567-73. S. (1985) 843-47. , Goluber, Int. , 14 (1971) 3. Heat 1759-70. Engineering Safin, 3. G. , Int. 3. Heat Mass T r a n s f e r 1 (1961) 167-74. 30. , Int. 3. Heat Mass T r a n s f e r 3 (1963) 559-70. , Bodies" in Advances 1964) 123-84. York, 32. 33. ,Int. V. in Mass Heat Transfer Transfer Mikhailov, (Pergamon P r e s s , O x f o r d , 34.
Edinburgh 21 (1857) 1 (1882) Sokolovskaya, 105-112. 123. 232. Heat Transfer, Soviet Heat Transfer, Soviet 93-104. and Sokolovskaya, 275-87. 28 Chapter 2 INTEGRAL EQUATION APPROACH TO HEAT AND MASS TRANSFER PROBLEMS Expressions for temperature and moisture distributions are derived for bodies of axisymmetric and spherical geometries by integral equations method. Approximate solutions, applicable for small values of generalised time, have also been worked out for the system. There place are through immobilise a some absorption of number the pores of heat the at of of processes solid diffusing times body in matter accompanied which which with by diffusion may the takes absorb evolution heat transfer medium diffusing different and matter produces through a the cross-effect body.
1 . 1 3 ) , we obtain the e x p r e s s i o n s for Q. 14) and v M* and moisture determine the values the of and hence the distributions are determined^ In order to simplify the calculations, we s h a l l determine an approximate solution of Xi(Fo) for small values of generalised Under the Laplace transformation, the integral time. 15) take the form 2 A X(s) 1 + 2 I J,k=l 1 (A M ' 7 1 ° ° ♦ B, M k ) ( l ' t ^(p x n ) I ° i L _ n=l 0 K n 35 * ) 4 s+Lu v . 16) n and A 2 _ J Mk J j,k=l A X2(s) + 2 (s) X| 2B2 + } 4 ~ s+Lu v p J " Xk(s) .