Non-Ideal Reactors, Residence Time Distribution & Dispersion Model Flashcards

1
Q

Define space time and write the equation

A

The time needed to fill one reactor volume (macromixing)

tao = V/v0

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2
Q

Define residence time

A

The amount of time molecules spend in the reactor (micromixing)

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3
Q

State the assumptions of the residence time distribution

A
  • Steady state
  • Without reaction
  • The fluid is incompressible so no density change
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4
Q

Why do we use the residence time distribution?

A

It allows the detection of non-ideal flows such as bypassing and short-circuiting by understanding the routes the fluid takes

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5
Q

What is the pulse experiment?

A

An experiment where a pulse input where N0 moles of an inert tracer is injected at t=0 and the concentration at the outlet is analysed. The vessel must be closed.

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6
Q

What is E(t)? What are the units?

A

The exit age distribution (1/time).

This shows the fraction of all the material leaving between a given time interval

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7
Q

Write the general equation for the exit age distribution

A

E (t) = C (t)/integral [C (t) dt]

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8
Q

Write the exit age distribution formulae in its discrete form

A

E (t) = C / sum [C delta (t)] = C / A
OR if the amount of tracer inputted is known:
E (t) = C v / N0

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9
Q

What is F (t)?

A

The cumulative distribution function.

This shows the fraction of fluid that leaves the reactor with an age less than a given value of t.

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10
Q

Write the general equation for the cumulative distribution function

A

F (t) = integral [E (t) dt]

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11
Q

How do you calculate the fraction of fluid that leaves the reactor with an age greater than a given value of t?

A

1 - F (t) = 1 - integral [E (t) dt]

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12
Q

Write the cumulative distribution function formulae in its discrete form

A

To find the F value for 1 specific time use:
F (t2) = F (t1) + (E (t1) + E (t2)/2) x delta (t2 - t1)

To find the fraction of fluid between 2 times (eg. 4 and 8 given in 2 min intervals):
F (t) = [ (E (4) + E (6))/2 ] x (6 - 4) + [(E (6) + E (8))/2 ] x (8 - 6)

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13
Q

Write the equation for the area under the C-curve

A
A = integral [ C(t) dt ] (infinity, 0)
A = sum [ Ci delta ti ] 
A = N0/v
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14
Q

Write the equation for the mean residence time of the C-curve

A

t = integral [ t E (t) dt ] (infinity, 0)

substituting in for E (t)

t = integral [ t C (t) dt ] (infinity, 0) / integral [ C (t) dt ] (infinity, 0)

t = sum [ ti Ci] / sum [ Ci ]

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15
Q

What is the difference between the C-curve and the E-curve?

A

The E-curve is the normalised version of the C-curve which neglects the amount of tracer and the volumetric flow rate. This allows two sets of experimental data to be more accurately compared

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16
Q

Write the equation for the area under the E-curve

A
A = N0/v
A = M/v
17
Q

Write the equation for the mean residence time of the E-curve

A

t = integral [ t E (t) dt ] (infinity, 0)

18
Q

Why would we use the E (theta) - curve? Define the units and necessary equations

A

To remove the effect of reactor volume

theta = ti/mean res time (t)

E (theta) = mean res time (t) x E

The units for E (theta) are dimensionless.

19
Q

Write the equation for the variance of the C-curve or E-curve?

A

variance = integral [ ti^2 E (t) dt ] (infinity, 0) - (mean res time (t))^2

20
Q

How do you diagnose reactor problems using the compartment model?

A

If reactor volume and volumetric flow rate is known we can use the compartment model.

Calculate V/v and compare this to the mean residence time observed from the data, if:

  1. mean res time (t) = V/v then the reactor has no dead spaces
  2. mean res time (t) ≠ V/v the reactor has dead spaces and the volume of dead space (Vd) can be calculated by:
    Vp = mean res time (t) x v
    Vd = V - Vp

If there is a bypass, the active volumetric flow rate (va) will be LESS than the total volumetric flow rate. To calculate the bypass volumetric flow (vb) use:
v = va + vb

21
Q

Draw the curves for the following diagnoses in a PFR:

  1. Stagnant backwaters
  2. Parallel paths/channelling
  3. Good flow
  4. Internal recirculation
  5. Late curve
A

See W9 notes

22
Q

What are the 2 potential reasons for the late curve diagnosis in a PFR?

A
  1. v or V has been measured incorrectly
  2. The tracer used is not inert
  3. The vessel is not closed
23
Q

Draw the curves for the following diagnoses in a CSTR:

  1. Stagnant fluud
  2. Time lag
  3. Good flow
  4. Internal recirculation
  5. Late curve
  6. Shortcircuiting
A

See W9 notes

24
Q

Outline the method for calculating a new conversion of reactant once a reactor diagnosis is improved

A
  1. Write the design equation
  2. Replace volume, V with Va (active volume) so that:
    k Va/v = ( CA0 / (1 - XA) CA0 ) - 1
  3. Calculate the RHS of the above equation (this is the ration for V/Va)
  4. Equate k V/v = n k Va/v so that it becomes:
    = n x (V/v) = number
  5. The number calculated in 4 = (CA0/CA2) - 1 so rearrange to find CA2/CA0
  6. The new conversion = 1 - the number in 5.
25
Q

What does the dispersion coefficient represent? What are the units?

A

The measure of the degree of backmixing/spreading. (m^2 / s)

  • Large D = rapid spreading
  • Small D = Slow spreading
26
Q

What does the dispersion coefficient represent? What are the units?

A

The measure of the degree of backmixing/spreading. (m^2 / s)

  • Large D = rapid spreading = CSTR = Broad RTD
  • Small D = Slow spreading = PFR = Narrow RTD
27
Q

Write the equation for the vessel dispersion number

A

VDN = D/uL = variance^2 (theta) /2

Where:
variance^2 (theta) = variance^2 / (mean res time)^2

28
Q

Write the equation for the vessel dispersion number when the vessel dispersion number is small?

A

VDN = D/uL = variance^2 (theta) /2

Where:
variance^2 (theta) the normalised variance = variance^2 / (mean res time)^2

29
Q

How do you calculate the normalised E-curve for the dispersion model and find the maximum when the vessel dispersion number is small?

A

E (theta) = mean res time (t) x E

The maximum occurs when theta = 1, therefore:

E (theta) max = 1/sqrt [4 pi (D/u L)]

30
Q

How can the vessel dispersion number be calculated from the normal distribution for small extents of dispersion (VDN < 0.01)?

A
  1. At the point of inflection (0.61 E (theta) max) where the width = 2 sqrt [2 (D/u L)]
  2. The width which includes 68% of the area where the shaded area = 0.68
31
Q

What is the additivity of variances when the vessel dispersion number is small? When is it used?

A

The increase in variance will always be the same therefore, the difference in variance can be used to calculate the vessel dispersion number in systems that have a small extent of dispersion.

delta variance ^2 = variance^2 (2) - variance^2 (1)

32
Q

How can the mean residence time be found for a packed bed when only bed voidage (BV), length and velocity of fluid is given when the vessel dispersion number is small?

A

t = V/v

V = L pi r^2 BV

v = velocity pi r^2

t = (L BV)/(velocity)

33
Q

What boundary condition gives a tracer curve that is identical to the E function?

A

close-close

laminar-laminar

34
Q

When the vessel dispersion number is large and the boundary condition is closed-closed, how do you calculate the normalised variance?

A

variance^2 (theta)
= variance^2 / (mean res time)^2
= 2 (D/u L)
= 2 (D/u L)^2 (1 - e^(u L/D))

35
Q

When the vessel dispersion number is large and the boundary condition is open-open, how do you calculate the normalised variance?

A

variance^2 (theta)
= variance^2 / (mean res time)^2
= 2 (D/u L) + 8 (D/u L)^2

36
Q

True or false: Tracer response curves for ‘closed’ vessels have larger deviations from plug flow

A

False

‘open’ vessels have a larger deviation

37
Q

How do you know whether a dispersion is large or small by looking at the E curve?

A

If the curve is unsymmetrical and broad then it is likely to be large