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LAB MANUAL
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Experiment – 4 Residence Time in Continuous Stirred Tank Reactor AIM: To study the residence time distribution in a CSTR and further to compare the results obtained with the expected theoretical results.
APPARATUS:
An overhead tank in order to maintain constant flow rate
Continuous Stirred Flow Reactor to analyze
Tracer (NaOH)
Stop Watch
Conductivity measuring instrument.
Injection to inject tracer
A beaker to collect effluent
EXPERIMENTAL PROCEDURE: 1. Fill the overhead tank with water and adjust the input and output flow rate in the tank so that its level remains constant. 2. From the overhead tank start the supply of water into the CSTR. 3. Adjust the flow rate of water into the CSTR until it comes equal to 1 mL/sec. 4. Now inject the tracer (NaOH) into the reactor and as soon as the tracer is injected start the stop watch. 5. Now keep on measuring the conductivity of the solution present in CSTR. 6. Stop your readings when the effluent streams contain negligible amount of the tracer.
THEORY: Residence Time is the time spent by an atom in a reactor. In an ideal CSTR the concentration of any substance in the effluent stream is identical to the concentration throughout the reactor. Consequently, it is possible to obtain the RTD from conceptual considerations in a fairly straight forward manner. But as we know that no reactor in the world is ideal and hence all the atoms/molecules entering the reactor don’t spend the same amount of time. To measure the non-ideality in a reactor we plot a residence time distribution of atoms in the reactor. To define it, Residence Time Distribution (RTD) of a reactor is a characteristic of the mixing that occurs in the chemical reactor. Non ideality comes into the picture and d ue to some disturbances in mixing the concentration of the exit effluents is not the same as that is there in the reactor. Experimentally, RTD is determined by injecting a tracer (which is normally an inert substance) in the reactor at some time t = 0 and then by measuring the tracer concentration in the effluent stream as a function of time. Some typical characteristics of a tracer are:
The tracer used should be a nonreactive species that is easily detachable. Should have similar physical properties to those of the reacting mixture and be b e completely soluble in the mixture. This is required so that the tracer’s behavior will honestly reflect that of the material flowing
It should not adsorb on the walls or other surfaces in the reactor.
Colored and radioactive materials along with inert gases are the most common types of tracers.
Here in this experiment we would use a pulse input of the tracer where an amount of tracer is suddenly injected in one shoot into the feed stream entering the reactor in as short a time as possible. The outlet co concentration ncentration is then measured as a function of time. A material balance on an inert tracer that has been injected as a pulse at time t = 0 into a CSTR for t > 0
Integrating the above the above equation with C = C o at t = 0, we get
We would further take C (t) as the measure of concentration of tracer as a function of time. Moving on we define a quantity E (t) as the residence-time distribution function. It is the function that describes in a quantitative manner how much time different fluid elements have spent in the reactor. Th e quantity E(t)dt is the fraction of fluid exiting the reactor that has spent between time t and t + dt inside the reactor. Mathematically it can be defined as:
An alternative way of defining the residence time distribution function can be:
As we know that the fraction of all the material that has resided for a time t in the react or between t = 0 and t = ∞ is 1 therefore,
Coming to the concept of space time or mean residen ce time (τ) , we know τ = V/vo. Now no matter what RTD exists for a particular reactor, ideal or non-ideal, non-ideal, the nominal space time τ, is equal to the mean residence time t m. As is the case with other variables described by distribution functions, the mean value of the variable is equal to the first moment of the RTD function, E (t). Thus the mean residence time is
OBSERVATIONS: Flow Rate (Q)
= 1 mL/s
Volume of Reactor (V)
= 870 mL
Time Constant Constant (τ)
= V/ Q
= 870/1
= 870 sec
Observation Tablet
C(Observed)
C(Theoretical)
C(t)dt
E(t)
E(t)dt
tE(t)dt
Experimental
Experimental
Experimental
Experimental
0
45.58
45.58
20
45
44.58413427
900
0.00096749
0.019349891
0.386998
24
44.5
44.38769363
178
0.00095674
0.003826979
0.091847
32.6
44
43.96839225
378.4
0.00094599
0.008135554
0.265219
43.7
43.54
43.43329221
483.294
0.0009361
0.010390763
0.454076
55.1
43
42.89079047
490.2
0.00092449
0.010539241
0.580712
66.8
42.5
42.34135501
497.25
0.00091374
0.010690815
0.714146
77.2
42
41.85913255
436.8
0.00090299
0.009391147
0.724997
89.6
41.5
41.29165836
514.6
0.00089224
0.011063838
0.99132
101.8
41
40.7411751
500.2
0.0008815
0.01075424
1.094782
114.7
40.5
40.16744242
522.45
0.00087075
0.011232612
1.288381
125.8
40
39.6805292
444
0.00086
0.009545946
1.20088
137.6
39.5
39.16967701
466.1
0.00084925
0.010021094
1.378902
149.1
39
38.67843515
448.5
0.0008385
0.009642696
1.437726
163.5
38.5
38.07240069
554.4
0.00082775
0.011919533
1.948844
178
38
37.4722095
551
0.000817
0.011846434
2.108665
188.8
37.5
37.03162583
405
0.00080625
0.008707451
1.643967
201.5
37
36.52048102
469.9
0.0007955
0.010102793
2.035713
216.1
36.5
35.94201162
532.9
0.00078475
0.011457286
2.475919
229.1
36
35.43504305
468
0.000774
0.010061944
2.305191
244
35.5
34.86322018
528.95
0.00076325
0.011372361
2.774856
257.2
35
34.36475544
462
0.0007525
0.009932944
2.554753
273.5
34.5
33.75957169
562.35
0.00074175
0.012090457
3.30674
287.2
34
33.25961715
465.8
0.000731
0.010014644
2.876206
300.7
33.5
32.77460276
452.25
0.00072025
0.00972332
2.923802
314.2
33
32.29705636
445.5
0.0007095
0.009578196
3.009469
330.12
32.5
31.74334492
517.4
0.00069875
0.011124038
3.672267
346.8
32
31.17396744
533.76
0.000688
0.011475776
3.979799
361
31.5
30.69777414
447.3
0.00067725
0.009616896
3.471699
376
31
30.20312349
465
0.0006665
0.009997444
3.759039
393.5
30.5
29.6367075
533.75
0.00065575
0.011475561
4.515633
409.8
30
29.11928205
489
0.000645
0.010513441
4.308408
427.6
29.5
28.5652049
525.1
0.00063425
0.011289587
4.827427
442.6
29
28.10700752
435
0.0006235
0.009352448
4.139393
458
28.5
27.64473862
438.9
0.00061275
0.009436297
4.321824
478.2
28
27.0506601
565.6
0.000602
0.012160332
5.815071
493.17
27.5
26.61920895
411.675
0.00059125
0.008850963
4.365029
513.6
27
26.04224698
551.61
0.0005805
0.011859548
6.091064
532.7
26.5
25.51496315
506.15
0.00056975
0.010882164
5.796929
552
26
24.99378747
501.8
0.000559
0.010788639
5.955329
569.6
25.5
24.52849291
448.8
0.00054825
0.009649146
5.496153
588.3
25
24.04432324
467.5
0.0005375
0.010051194
5.913117
606.7
24.5
23.57797153
450.8
0.00052675
0.009692146
5.880225
629.2
24
23.02094759
540
0.000516
0.011609935
7.304971
650.3
23.5
22.51151113
495.85
0.00050525
0.010660715
6.932663
671.7
23
22.00729833
492.2
0.0004945
0.010582241
7.108091
693.4
22.5
21.50852569
488.25
0.00048375
0.010497316
7.278839
713.7
22
21.05306117
446.6
0.000473
0.009601846
6.852838
740.5
21.5
20.46780673
576.2
0.00046225
0.01238823
9.173485
760.6
21
20.04054648
422.1
0.0004515
0.009075099
6.90252
786.3
20.5
19.50843301
526.85
0.00044075
0.011327211
8.906586
809.4
20
19.04338277
462
0.00043
0.009932944
8.039725
834.5
19.5
18.55187153
489.45
0.00041925
0.010523116
8.78154
862.3
19
18.02378585
528.2
0.0004085
0.011356236
9.792483
887.4
18.5
17.56127028
464.35
0.00039775
0.009983469
8.85933
915.3
18
17.06257888
502.2
0.000387
0.010797239
9.882713
942.4
17.5
16.5932598
474.25
0.00037625
0.010196318
9.60901
972.4
17
16.09048641
510
0.0003655
0.010964938
10.66231
1001.1
16.5
15.62545755
473.55
0.00035475
0.010181268
10.19247
1031.6
16
15.14779148
488
0.000344
0.010491941
10.82349
1064.6
15.5
14.649489
511.5
0.00033325
0.010997188
11.70761
1096.1
15
14.19114823
472.5
0.0003225
0.010158693
11.13494
1129.9
14.5
13.71745223
490.1
0.00031175
0.010537091
11.90586
1164.2
14
13.25519836
480.2
0.000301
0.010324242
12.01948
1200.7
13.5
12.78290512
492.75
0.00029025
0.010594066
12.72029
1238.4
13
12.3154473
490.1
0.0002795
0.010537091
13.04913
1278.2
12.5
11.84344461
497.5
0.00026875
0.01069619
13.67187
1318.6
12
11.38590739
484.8
0.000258
0.010423141
13.74395
1361
11.5
10.92803079
487.6
0.00024725
0.010483341
14.26783
1403
11
10.49594965
462
0.0002365
0.009932944
13.93592
1452.8
10.5
10.00993463
522.9
0.00022575
0.011242287
16.33279
1501.9
10
9.557229631
491
0.000215
0.010556441
15.85472
1553.1
9.5
9.111599587
486.4
0.00020425
0.010457541
16.24161
1606.5
9
8.673932717
480.6
0.0001935
0.010332842
16.59971
1664.1
8.5
8.231006842
489.6
0.00018275
0.010526341
17.51688
1772.8
8
7.470971702
869.6
0.000172
0.018696295
33.14479
1784.2
7.5
7.396626434
85.5
0.00016125
0.00183824
3.279787
1849
7
6.992048991
453.6
0.0001505
0.009752345
18.03209
1921
6.5
6.576484751
468
0.00013975
0.010061944
19.32899
2070
5.5
5.818364213
819.5
0.00011825
0.017619151
36.47164
2170
5
5.377696367
500
0.0001075
0.01074994
23.32737
2273
4.5
4.973776277
463.5
9.6749E-05
0.009965194
22.65089
2391
4
4.566152904
472
8.6E-05
0.010147943
24.26373
2531
3.5
4.149047932
490
7.525E-05
0.010534941
26.66394
2704
3
3.718236566
519
6.45E-05
0.011158437
30.17241
2984
2.5
3.17935888
700
5.375E-05
0.015049916
44.90895
3763
2
2.339727553
1558
4.3E-05
0.033496812
126.0485
5400
1.8
1.848318453
2946.6
3.87E-05
0.063351544
342.0983
Integral[ C(t)dt ] Integral[ E(t)dt ] Residence Time
46511.889 1 1231.0796
Graph of C (t) vs time –
50 45 40 35
y t i v i t c u d n o C
30 25
Observed Theoritical
20 15 10 5 0 0
10 00
20 00
30 00 Time
4 00 0
50 00
6 00 0
RESULT: The residence time for the flow reactor is observed to be 1231.08 seconds.
CONCLUSION: For a CSTR initially the concentration shoots up very fast and reaches a maximum and then starts decaying exponentially. The reason for the instant shoot up is that both the inlet and outlet pipes are at the same level and hence some of tracer injected gets immediately removed from the reactor and the rest is caught up in the mixture and exists slowly. In a CSTR it is very much possible that a volume such as dead volume develops where some of the material is trapped and is never able to exit from the reactor. This volume might be found at one of the corners of the reactor.