Download presentation
Presentation is loading. Please wait.
1
Exercises 5
2
5.1) Describe the general elution problem
Exercise 5.1 5.1) Describe the general elution problem
3
Exercise 5.1 5.1) Describe the general elution problem
Elution patterns typically follow an exponential function Too low eluent strength = too long time “The general elution problem in chromatography” Too high eluent strength = too low resolution
4
Exercise 5.1 The general elution problem is solved by applying a gradient of temperature in GC or of elution strength in LC Solvent strength Gradient elution: The first compounds eluted with low eluent strength, the last compounds eluted with high eluent strength Time Gradient elution is suitable for a large range of analyte properties Detector response Time
5
Exercise 5.2
6
Exercise 5.2 A situation where k is not constant
7
Exercise 5.2 A situation where k is not constant
8
Exercise 5.2 A situation where k is not constant
9
Exercise 5.2 A situation where k is not constant
10
Exercise 5.2 A situation where k is not constant
Valid, but not constant
11
Exercise 5.2 A situation where k is not constant
Valid, but not constant
12
Exercise 5.2 A situation where k is not constant
13
Exercise 5.2 A situation where k is not constant
14
Exercise 5.2 A situation where k is not constant
Part of the expression is valid but not the relationship involving k Mathematically valid but not very useful
15
Exercise 5.2 A situation where k is not constant
Part of the expression is valid but not the relationship involving k Mathematically valid but not very useful Underlying factors depend on k Underlying factors depend on k
16
Exercise 5.2 A situation where k is not constant
Part of the expression is valid but not the relationship involving k Mathematically valid but not very useful Underlying factors depend on k Underlying factors depend on k
17
Exercise 5.2 A situation where k is not constant 2
18
Exercise 5.2 A situation where k is not constant
The van Deemter eqation is not valid since it includes H, but the underlying relationships will be similar or identical as in isothermal chromatograpgy
19
Exercise 5.2 A situation where k is not constant
Strictly not valid since the van Deempter equation is not valid, but the same things that give low H will be good also in programmed chromatography
20
Exercise 5.2 A situation where k is not constant
The van Deemter eqation is not valid since it includes H, but the underlying relationships will be similar or identical as in isothermal chromatograpgy
21
Exercise 5.2 A situation where k is not constant
22
Exercise 5.2 A situation where k is not constant
23
Exercise 5.2 A situation where k is not constant
24
Exercise 5.2 A situation where k is not constant
25
Exercise 5.2 A situation where k is not constant
26
Exercise 5.2 A situation where k is not constant
27
Exercise 5.3 5.0 s 3.0 s 10% 3.4 s 5.6 s 5%
28
Exercise 5.3 wright,10% wleft,10% Af = w5% 2∙wleft,5% Tf = (Eq 24)
29
Exercise 5.3 wright,10% wleft,10% Af = w5% 2∙wleft,5% Tf =
(Eq 24) Tf = w5% 2∙wleft,5% (Eq 25) Af = 5.0 s / 3.0 s = 1.7 Tf = ( ) s / (2 ∙ 3.4) s = 1.3
30
Exercise 5.3 wright,10% wleft,10% Af = w5% 2∙wleft,5% Tf =
(Eq 24) Tf = w5% 2∙wleft,5% (Eq 25) 5.0 s 3.0 s 10% 5% 5.6 s 3.4 s Af = 3.0 s / 5.0 s = 0.60 Tf = ( ) s / (2 ∙ 5.6) s = 0.80
31
Exercise 5.3 wright,10% wleft,10% Af = w5% 2∙wleft,5% Tf =
(Eq 24) Tf = w5% 2∙wleft,5% (Eq 25) 5.0 s 3.0 s 10% 5% Both factors give value 1 for symmetric peaks Fronting peaks have values below 1 Tailing peaks have values above 1 5.6 s 3.4 s Af = 3.0 s / 5.0 s = 0.60 Tf = ( ) s / (2 ∙ 5.6) s = 0.80
32
Exercise 5.4
33
Exercise 5.4 Homologous series of alkanes.
Can be used to calculate retention indices: n-pentane ≡ 500 n-hexane ≡ 600 n-heptane ≡ 700
34
Exercise 5.4 Homologous series of alkanes.
Can be used to calculate retention indices: n-pentane ≡ 500 n-hexane ≡ 600 n-heptane ≡ 700 Differences between homologs z and z+1 are 100 retention index units
35
Exercise 5.4 Table of Kovats’ retention indices
36
Exercise 5.4 (Eq 22) This is isothermal chromatography, so we have to apply the equation with log of adjusted retention times
37
Exercise 5.4 references 535 3.99 – 3.51 4.59 – 3.51
(Eq 22) 3.99 – 3.51 4.59 – 3.51 log 1.08 – log 0.48 log 4.83 – log 0.48 For compound A: I = 100 + 5 = 535 First reference has five carbons 8.34 – 3.51
38
Exercise 5.4 535 log 1.08 – log 0.48 log 4.83 – log 0.48
(Eq 22) log 1.08 – log 0.48 log 4.83 – log 0.48 For compound A: I = 100 + 5 = 535
39
Exercise 5.4 references 535 635 log 10.82 – log 4.83
(Eq 22) log – log 4.83 log – log 4.83 I = 100 + 6 = 635 First reference has six carbons
40
Exercise 5.4 535 635 678 log 29.12 – log 4.83 log 48.33 – log 4.83
(Eq 22) log – log 4.83 log – log 4.83 I = 100 + 6 = 678
41
Exercise 5.4 691 535 635 678 log 39.29 – log 4.83 log 48.33 – log 4.83
(Eq 22) log – log 4.83 log – log 4.83 I = 100 + 6 = 691
42
Exercise 5.4 691 535 635 678 635 535 678 691
43
Exercise 5.5
44
Exercise 5.5
45
Exercise 5.5 A series of homologs
we can calculate the separation number
46
The separation number:
Exercise 5.5 The separation number: SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1 A series of homologs we can calculate the separation number
47
Exercise 5.5 SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1 26.61 – 24.21
The separation number: SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1 Calculated for the region between 18 and 19: Program A Program B 26.61 – 24.21 18.63 – 17.29 SN = – 1 = 18.7 SN = – 1 = 15.7 A has higher separation efficiency than than B A series of homologs we can calculate the separation number
48
Exercise 5.5 A B SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1
The separation number: SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1 Calculated for the region between 18 and 19: Program A Program B 26.61 – 24.21 18.63 – 17.29 SN = – 1 = 18.7 SN = – 1 = 15.7 A has higher separation efficiency than than B 23 SN A B 18 13 8 Same pattern for the other chain lengths 3 Chain length 14 15 16 17 18 19 20 21
49
The separation number:
Exercise 5.5 The separation number: SN = tR(z+1) – tR(z) wh(z) + wh(z+1) – 1 This can also be solved using the peak capacity. Use for instance the number of peaks between 14:0 and 20:0 (first and last peak) (Eq. 21)
50
Exercise 5.5
51
Retention index for temperture programmed conditions
Exercise 5.5 Retention index for temperture programmed conditions tR(i) – tR(z) tR(z+1) – tR(z) IT = B + z
52
Retention index for temperture programmed conditions
Exercise 5.5 Retention index for temperture programmed conditions tR(i) – tR(z) tR(z+1) – tR(z) IT = B + z For 18:1 n-9 Program A Program B 25.14 – 24.21 26.61 – 24.21 17.85 – 17.30 18.63 – 17.30 IT = 1 + 18 = 18.39 IT = 1 + 18 = 18.41 The difference in retention indices between homologs is 1 in this case (ECL values)
53
Retention index for temperture programmed conditions
Exercise 5.5 Retention index for temperture programmed conditions tR(i) – tR(z) tR(z+1) – tR(z) IT = B + z For 18:1 n-9 Program A Program B 25.14 – 24.21 26.61 – 24.21 17.85 – 17.30 18.63 – 17.30 IT = 1 + 18 = 18.39 IT = 1 + 18 = 18.41 Difference in retention index 18.41 – 18.39 18.40 ∙ 100 % = 0.15 % Difference in retention time 25.13 – 17.85 21.5 ∙ 100 % = 33 %
54
Retention index for temperture programmed conditions
Exercise 5.5 Retention index for temperture programmed conditions tR(i) – tR(z) tR(z+1) – tR(z) IT = B + z For 18:1 n-9 Program A Program B 25.14 – 24.21 26.61 – 24.21 17.85 – 17.30 18.63 – 17.30 IT = 1 + 18 = 18.39 IT = 1 + 18 = 18.41 Difference in retention index Tells us that the selectivity is the same (which makes sense since the stationary phase is the same) 18.41 – 18.39 18.40 ∙ 100 % = 0.15 % Difference in retention time 25.13 – 17.85 21.5 ∙ 100 % = 33 % Tells nothing about selectivity
55
Retention index for temperture programmed conditions
Exercise 5.5 Retention index for temperture programmed conditions tR(i) – tR(z) tR(z+1) – tR(z) IT = B + z For 18:2 n-6 For 18:2 you do the same, but remember to change the references since it elutes between 19:0 and 20:0
57
20 cm/s carrier gas velocity on a 25 m × 0
20 cm/s carrier gas velocity on a 25 m × 0.25 mm column requires an inlet pressure of 65 kPa (9.40 psi / bar) The length may vary from to m The diameter may vary from to mm.
58
Apply 65 kPa with these dimensions:
0.265 0.260 0.255 Diameter (mm) 0.250 0.245 0.240 0.235 23 24 25 26 27 Length (m)
59
Apply 65 kPa with these dimensions:
0.265 0.260 0.255 Diameter (mm) 20 cm/s 0.250 0.245 0.240 0.235 23 24 25 26 27 Length (m)
60
Apply 65 kPa with these dimensions:
0.265 0.260 23.3 21.1 0.255 Diameter (mm) 20.0 cm/s 0.250 0.245 19.1 17.3 0.240 0.235 23 24 25 26 27 Length (m)
61
Apply 65 kPa with these dimensions:
The carrier gas velocity is within 17.3 to 23.3 cm/s 0.265 0.260 23.3 21.1 0.255 Diameter (mm) 20.0 cm/s 0.250 0.245 19.1 17.3 0.240 0.235 23 24 25 26 27 Length (m)
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.