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Spring 2009 Turbidity Profiles

Methods

  • Hot-swapping Baffle Configurations

Two adjustable baffle configurations were built this semester. Each consists of two 6' rows of baffles, one row for each of the first two channels of the flocculator. While one configuration (2 rows) is in the flocculator and being tested, the other configuration (which is not in use) can have its baffle spacing altered. Because that is possible, instead of needing to wait between experiments while baffle spacing is readjusted, the new baffle spacing can be ready on the second baffle configuration and the two configurations can be simply swapped. Then, while the next experiment is running, the first baffle configuration can have its spacing altered to be ready for the subsequent experiment. Since each configuration also has different length spacers (and new spacer of other lengths can be readily fabricated), flocculator arrangements where one channel has a certain baffle spacing while the other channel has a different baffle spacing, echoing the current plant design, can be tested as well.

  • PAC dosing

Polyaluminum chloride (PAC) is the coagulant of choice of the Cornell Water Treatment Plant as well as many other plants across the United States. According to plant workers PAC is much more forgiving than alum in terms of dosing and forms flocs better in colder water, which is important when testing in Ithaca. Dosing with PAC was set up at the Pilot Plant. Our goal was to collect turbidity profiles of the tank based upon energy dissipation (the spacing of the baffles). To facilitate this goal and remove a large source of potential error, we eliminated alum dosing in favor of dosing the same proportion of PAC that the treatment plant is dosing (the plant doses PAC in ppm of the total flow). This should make the profiles more comparable and the effects of baffle spacing more clear, since temperature and non-optimal dosing effects have been greatly reduced by adopting PAC.

  • Normalizing Data

In previous tests, many data samples needed to be collected in one sitting to avoid having large fluctuations in turbidity, which required experimenting and determining new alum dosages, and often resulted in data that could not be compared between days of testing. The new adjustable baffle system will do much to ameliorate this problem by allowing the pilot plant team to perform experiments faster. In addition, to keep our results consistent and relevant to one another every day of experimentation will start with a turbidity profile for a "normalizing" configuration, a configuration with .102 m baffle spacing so profiles collected at different times can be compared based upon the results of the normalizing setup.

Calculations


Unknown macro: {float}
Equation for energy dissipation:

Unknown macro: {float}
Equation for flocculator residence time:


Length of flocculator channel = 1.8288 m
K baffle = 4
Π cell = 4
w = .305 m
h = .764 m

 

Q 50 = 50 L/min

 

 

Q 100 = 100 L/min

 

 

b (m)

ε (mW/kg)

N (#baffles/channel)

θ channel (residence time/channel) (sec)

ε (mW/kg)

N (#baffles/channel)

θ channel (residence time/channel) (sec)

.051

1.507

34

484.9

12.06

34

242.4

.076

.306

23

488.8

2.445

23

244.4

.102

.094

16

456.3

.754

16

228.2

.127

.039

13

461.7

.314

13

230.8

.152

.019

11

467.5

0.153

11

233.8

.178

.01

9

448.0

0.081

9

224.0

.203

.006

8

454.1

0.048

8

227.1

Turbidity Profiles

Configuration

1st channel

2nd channel

θ flocculator (s) at Q 50

θ flocculator (s) at Q 100

1

.152 m

.152 m

935.1

467.7

2

.076 m

.076 m

977.6

488.8

3

.102 m

.102 m

9127

456.3

4

.127 m

.127 m

923.3

461.7

5

.051 m

.051 m

969.7

484.9

6

.178 m

.178 m

895.9

448.0

7

.203 m

.203 m

908.2

454.1

8

.051 m

.076 m

973.7

486.9

9

.051 m

.102 m

941.2

470.6

10

.051 m

.152 m

952.4

476.2

11

.051 m

.203 m

939.0

469.5

12

.076 m

.102 m

945.1

472.6

[13]

.102 m

.152 m

923.9

461.94

Results and Findings

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