Fluid catalytic cracking
bài giảng công nghệ chế biến dầu mỏ chương 5 cracking xúc tác FCC (catalytic cracking)
... hoàn xúc tác 6.2 Cracking xúc tác lớp sôi Hơi; Xúc tác; Hơi hydrocacbon; Bình phản ứng Mô hoạt động vùng sục xúc tác 6.2 Cracking xúc tác lớp sôi 6.2 Cracking xúc tác lớp sôi Công nghệ FCC ngày ... UOP) 6.2 Cracking xúc tác lớp sôi Sơ đồ thiết bị tái sinh xúc tác với hệ thống làm mát xúc tác (UOP) 6.2 Cracking xúc tác lớp sôi Hệ thống làm...
Chapter 5 catalytic cracking
... trung hòa chúng cấu tử sản phẩm cracking xúc tác 4 Hóa học trình cracking XT 4.1 Phản ứng mong muốn Phản ứng cắt mạch (cracking ): xảy theo chế ion cacbonium Hoạt tính cracking hydrocacbon giảm dần ... trình cracking XT 4.1 Phản ứng mong muốn Phản ứng isomer hoá: Thường xảy trước phản ứng cracking 4 Hóa học trình cracking XT 4.2 Phản ứng không mong muốn Phản ứng chuyển vị hydro...
Cracking xúc tác
... công nghệ cracking Các trình cracking, tiên, đợc thực mặt chất xúc tác, nhng sau, 4-5 thập kỷ gần đây, nhiều chất xúc tác cracking liên tục xuất cải tiến Hầu hết chất xúc tác cracking xúc tác axit ... nghệ cracking xúc tác thập kỷ qua phát minh phát triển liên tục xúc tác zeolit Các zeolit (dạng axit, H-zeolit) xúc tác cho phản ứng cracking dầu mỏ nhanh h...
Introduction to fluid mechanics - P1
... beginning of fluid mechanics Fig 1.3 Ancient Greek ship depicted on old vase inclination or supply pressure had to be adjusted to overcome friction with the wall of the conduit This gave rise to much ... was the first to find the least resistive ‘streamline’ shape 4 History of fluid mechanics Leonardo da Vinci (145 2-1 519 ) An all-round genius born in Italy His unceasing z...
Introduction to fluid mechanics - P2
... Kinematic viscosity B Y units 0 1 0 0 m kg -3 -1 1 1 -1 -1 -2 -2 -2 -2 -1 -1 S mls m/s2 kg I m3 N = kg m/s2 Pa = N/m2 J Pa s m2/s Characteristics of a fluid 2.2.2 Dimension All physical quantities ... proportional to the velocity gradient duldy Such fluids are called Newtonian fluids On the other hand, liquid which is not subject to Newton's law of viscosit...
Introduction to fluid mechanics - P3
... semiconductor strain gauge PGM-C Pressure range (MPa) Natural frequency (kHz1 Response frequency (kHz1 PE-J, P (a) Small size 0. 2-1 o 2 5-4 0 5-8 (b) For indicating pressure of an engine 5-2 0 2 5-4 0 5-8 ... pdAor ( ) p+-dz dA-pgdAdz=O 24 Fluid statics Fig 3.4 Balance of vertical minute cylinder dp _ - -PS &" (3.6) Since p is constant for liquid, the following equation ens...
Introduction to fluid mechanics - P4
... direction moves to A‘B’ while rotating by dq, and AD in the y direction rotates by de, Thus av de - - dxdt - ax at4 d = dydt E aY de - L = - d av d~ t I - dx ax de = dt dE2 dy au - ay The angular ... case of two-dimensional flow where w = V is an operator which represents a a a ax ay az i-+j-+k- where i,j , k are unit vectors on the x, y z axes 50 Fundamentals of f...
Introduction to fluid mechanics - P5
... momentum: - (D’ increase in momentum: R - d2)pu: 71 -p[D2u: 71 + -d’pui - (0’ - d2)u: - d’ui] 71 force acting on the fluid: -D’(p, - p ) By the law of momentum, ~ [ D ’ u - (D’ - d2)u: - d ’ ~ ... respectively Then from Bernoulli’s equation Pl u: 2g P2 -+ -+ z PS VI - PS 29 +-+ z2 Assuming that the pipe line is horizontal, z1 = 22 v2 - v: -...
Introduction to fluid mechanics - P6
... following equation: a u a u au du = -dt + dx -dy at ax ay + Therefore, du _ - -au + -audx- ~ -audy- + ~ -+ +u dt at axdt aydt at au ax aU ay Substituting this into eqn (6.4), Next, the force F acting ... d y = -h3 dP 12pdx From this equation, the mean velocity u is Q = - = -h2 dP = - u1 h 12pdx 1.5 (6.23) (6.24) The shearing stress z due to viscosity becomes ldp z = p - d...
Introduction to fluid mechanics - P7
... efficiency q for a diffuser is therefore P2-P1 - q=-P2th - PI hs (0: - U:)/2s (7.31) Substituting in eqn (7.28), the above equation becomes q = - c - 02 - - + 02 - Al/A2 + Al/A2 (7.32) Convergent pipe ... losses in pipe lines 125 P P -+ - v: = -+ -+ P9 29 h, 29 P9 Therefore €72 - PI - - P9 hs 29 (7.29) Putting pzth p for the case where there is...
Introduction to fluid mechanics - P8
... (8.6) and (8.7) (-) v =- A 2'3i1,2 n s Q = -1 i A5/3 - ll2 n s2I3 A = r2(;) - ?cos(;) = r2(e- sin e) sin(;) s = re ( m = - 1-2 r si:e> i.e n -T)] Z( 1-7 ) sin 'I3 v=-i112[;(1 Q = -i'121 n sine 'I3 ... cross-sections are uniform and whose banks are covered with wild grass Bending river with large stones and wild grass 0.01 0-0 .013 0.01 2-0 .018 0.01 3-0 .017 0.01...
Introduction to fluid mechanics - P9
... Bernoulli’s equation produces the following result: u2 Pd +P2 +2 pm -= p P-Pm= - -Po, PU2/2 p(U2 - Ui) (1 -4 sin28) - pu’ - -4 sinz0 (9.6) The drag of a body 151 Table 9.2 Drag coefficients for ... Drag and lift L=2 -( p-p,)rodBsin8 1n/2 ( I', u+roo = - r o p u r - 2U sin [I -XI2 (k) sin dB = - r o p U r [l - r w - z4s r n B - s i n io -4 2...
Từ khóa:
- applications for fluid catalytic cracking
- application of 1h nmr for fluid catalytic cracking feed characterization
- fluid catalytic cracking fcc
- deep oil fluid catalytic cracking
- s amp w fluid catalytic cracking process
- residue fluid catalytic cracking
- hds and fluid catalytic cracking fcc
- uop fluid bed catalytic cracking
- deep catalytic cracking the new light olefin generator