Difference between revisions of "Isothermal reactor design - 2013"

From Introduction to Reactor Design: 3K4
Jump to navigation Jump to search
m
m
Line 7: Line 7:
| vimeoID4 = 59455740
| vimeoID4 = 59455740
| vimeoID5 = 59734705
| vimeoID5 = 59734705
| vimeoID6 = 60514877
| course_notes_PDF =  
| course_notes_PDF =  
| course_notes_alt = Course notes
| course_notes_alt = Course notes
Line 27: Line 28:
| video_download_link5_MP4_size = 243 M
| video_download_link5_MP4_size = 243 M
| video_notes5 =
| video_notes5 =
| video_download_link6_MP4 = http://learnche.mcmaster.ca/media/3K4-2013-Class-07A.mp4
| video_download_link6_MP4_size = 353 M
| video_notes6 =
}}__NOTOC__
}}__NOTOC__



Revision as of 00:44, 26 February 2013

Class date(s): 04 February to 14 February
Download video: Link (plays in Google Chrome) [291 M]

Download video: Link (plays in Google Chrome) [304 M]

Download video: Link (plays in Google Chrome) [393 M]

Download video: Link (plays in Google Chrome) [M]

Download video: Link (plays in Google Chrome) [243 M]

Download video: Link (plays in Google Chrome) [353 M]

  • F2011: Chapter 5 and 6
  • F2006: Chapter 4

04 February 2013 (05A)

06 February 2013 (05B)

07 February 2013 (05C)

to see the effect on pressure drop in the packed bed.

11 February 2013 (06A)

14 February 2013 (06C): midterm review

25 February 2013 (07A)

The example covered in class is based on example 4-8 in F2006 and example 6-2 in F2011. <rst> <rst-options: 'toc' = False/> <rst-options: 'reset-figures' = False/> The 3 ODE's are:

.. math::

\dfrac{dF_A}{dV} &= r_A\\ \dfrac{dF_B}{dV} &= r_B - R_B \\ \dfrac{dF_C}{dV} &= r_C

where :math:`-r_A = r_B = r_C` and :math:`-r_A = k\left(C_A - \dfrac{C_B C_C}{K_C} \right)`, and :math:`R_B = k_\text{diff}C_B`.

  • :math:`k = 0.01\,\text{s}^{-1}`
  • :math:`k_\text{diff} = 0.005\,\text{s}^{-1}`
  • :math:`K_C = 50\,\text{mol.m}^{-3}`

We derived earlier in the course that

.. math:: C_A = C_\text{TO}\left(\dfrac{F_A}{F_T}\right)\left(\dfrac{P}{P_0}\right)\left(\dfrac{T_0}{T}\right)

Assuming isothermal and isobaric conditions in the membrane:

.. math:: C_A = C_\text{T0}\left(\dfrac{F_A}{F_T}\right)

where :math:`F_T = F_A + F_B + F_C` and :math:`C_\text{T0} = \dfrac{P_0}{RT_0}`. Similar equations can be written for :math:`C_B` and :math:`C_C`.

Using all of the above derivations, we can set up our numerical integration as shown below. </rst>

MATLAB Python

In a file called membrane.m:

sdfsdf

In a separate file (any name), for example: ode_driver.m, which will "drive" the ODE solver:

asdas

File:Plots-MATLAB.png

asdasd

File:Plots-Python.png

and in Polymath:

d(FA)/d(V) = rA
d(FB)/d(V) = rB - kDiff * CB
d(FC)/d(V) = rC

FA(0) = 0.25  # mol/s
FB(0) = 0.0   # mol/s
FC(0) = 0.0   # mol/s

# Independent variable	
V(0) = 0
V(f) = 0.4  #m^3

# Constants
kDiff = 0.005  # s^{-1}
k = 0.01       # s^{-1}
KC = 50        # mol.m^{-3}
P0 = 830600    # Pa
T0 = 500       # K
R  = 8.314     # J/(mol.K)

# Algebraic equations
FT = FA + FB + FC
CT0 = P0 / (R * T0)
CA = CT0 * FA / FT
CB = CT0 * FB / FT
CC = CT0 * FC / FT
rA = -k * (CA - CB * CC / KC)
rB = -rA
rC = -rA