a digital microfluidic device for antibiotic testing in milk

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A Digital Microfluidic Device for Antibiotic Testing in Milk by Rahul Eswar A Thesis presented to The University of Guelph In partial fulfilment of requirements for the degree of Master of Applied Science in Engineering Guelph, Ontario, Canada © Rahul Eswar, January, 2021

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Page 1: A Digital Microfluidic Device for Antibiotic Testing in Milk

A Digital Microfluidic Device for Antibiotic Testing in Milk

by

Rahul Eswar

A Thesis

presented to

The University of Guelph

In partial fulfilment of requirements for the degree of

Master of Applied Science

in

Engineering

Guelph, Ontario, Canada

© Rahul Eswar, January, 2021

Page 2: A Digital Microfluidic Device for Antibiotic Testing in Milk

ABSTRACT

A DIGITAL MICROFLUIDIC DEVICE FOR ANTIBIOTIC TESTING IN MILK

Rahul Eswar

University of Guelph, 2021

Advisor:

Dr. Christopher Collier

Co-Advisor:

Dr. Ashutosh Singh

Worldwide, milk is tested to meet limits for antibiotic residue content which can

invoke allergic reaction and antibiotic resistance in human consumers. Dairy farmers

are responsible for collecting milk and shipping it to off-site laboratories for testing. Non-

compliant milk results in penalties including fines and loss of licensure for offending

dairy farmers. Modern on-site testers require long response times and manual

preparation procedures which are unavailable during milk collection. An appealing

technology to address this issue is digital microfluidics which handles sample in discrete

droplets to leverage reconfigurability and automation. This thesis demonstrates the

fundamental functionalities required by an on-site digital microfluidic dairy tester. Design

of an integrated digital microfluidic device for milk droplet actuation is detailed. A label-

free method for antibiotic detection in milk droplets is demonstrated using lock-in

amplified fluorescence spectroscopy. This work provides the foundation for

development of a full on-site digital microfluidic dairy testing solution.

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ACKNOWLEDGEMENTS

There are a number of individuals I must thank as this work would not have been

possible without their collaboration.

I want to first extend the utmost gratitude to my advisor, Dr. Christopher Collier.

His guidance, support and confidence in me have been invaluable to my growth and to

the completion of this work. I feel very fortunate to have worked as part of his team.

I want to also thank my co-advisor, Dr. Ashutosh Singh, for providing access to

his Food Research Lab and always encouraging my work.

For their willingness to serve on my advisory committee, I am grateful to Dr.

Christopher Collier, Dr. Ashutosh Singh and Dr. Abdallah Elsayed. I greatly appreciate

their time and commitment to oversee my progress.

Many thanks go to Larry Wood and Norwell Dairy Systems for providing the

inspiration for this work. This project is a direct product of their support.

For laying the foundation on which this work is built, I want to thank Rick Bosma.

His advice and technical assistance has been instrumental in accomplishing this work.

I am very grateful to David Wright and Jacqueline Fountain for their technical and

administrative support of my work. I feel fortunate to have completed this work at the

University of Guelph due in large part to exceptional staff like them.

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Special thanks go to Harrison Brodie, Jasen Devasagayam, Iasmin de Franca

Albuquerque, Michelle Del Rosso and Sydney Lepard for their collaboration and advice.

I would like to thank all my colleagues in the Applied Optics and Microsystems

Laboratory for their advice and friendships throughout this undertaking.

For their technical support, I want to thank Saipriya Ramalingam and Benjamin

Dyer. Their ever present willingness to lend their expertise has been critical to the

completion of this work.

Lastly, thank you to my father, mother and brother, Eswar, Rajani and Aditya.

They have inspired and believed in me always.

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v

TABLE OF CONTENTS

Abstract ............................................................................................................................ii

Acknowledgements ......................................................................................................... iii

Table of Contents ............................................................................................................ v

List of Figures ................................................................................................................ viii

1 Introduction .............................................................................................................. 1

1.1 Background ........................................................................................................ 1

1.2 Thesis Scope ..................................................................................................... 3

2 Literature Review ..................................................................................................... 4

2.1 Introduction ........................................................................................................ 4

2.2 Regulated Antibiotics in Dairy ............................................................................ 4

2.3 Laboratory Detection Methods ........................................................................... 5

2.3.1 High Pressure Liquid Chromatography ........................................................ 5

2.3.2 Immunoassays ............................................................................................ 7

2.4 On-site Detection Methods ................................................................................. 9

2.4.1 Lateral Flow Assay ...................................................................................... 9

2.4.2 Prepared Incubated Test ........................................................................... 11

2.4.3 Microchip Capillary Electrophoresis ........................................................... 12

2.5 Actuation on Digital Microfluidic Devices .......................................................... 15

2.5.1 General Digital Microfluidic Design ............................................................ 15

2.5.2 Biofouling ................................................................................................... 16

2.5.3 Filler Medium ............................................................................................. 17

2.6 Detection on Digital Microfluidic Devices ......................................................... 18

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2.6.1 Fluorescence Spectroscopy ...................................................................... 18

2.6.2 Surface Plasmon Resonance .................................................................... 20

2.6.3 Impedance Spectroscopy .......................................................................... 21

2.6.4 Electrochemical Detection ......................................................................... 21

3 An Integrated Digital Microfluidic Device for Dairy Applications ............................. 23

3.1 Chapter Introduction ......................................................................................... 23

3.2 Background ...................................................................................................... 24

3.3 Electrowetting Actuation ................................................................................... 28

3.4 General DMF Design ....................................................................................... 30

3.5 DMF Prototype Design ..................................................................................... 32

3.6 Closed Configuration Experiments ................................................................... 34

3.7 Open Configuration Experiments ..................................................................... 39

3.8 Methods ........................................................................................................... 44

3.8.1 Reagents ................................................................................................... 44

3.8.2 Digital Microfluidic Device Printed Circuit Board ........................................ 44

3.8.3 Dielectric Coating ...................................................................................... 45

3.8.4 Statistical Analysis ..................................................................................... 45

3.9 Chapter Conclusion .......................................................................................... 46

4 Label-free Antibiotic Detection in Milk Droplets ...................................................... 47

4.1 Chapter Introduction ......................................................................................... 47

4.2 Lock-In Amplification ........................................................................................ 51

4.3 Experimental Setup .......................................................................................... 53

4.4 Rhodamine Pilot Experiment ............................................................................ 55

4.5 Antibiotic Detection .......................................................................................... 57

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4.6 Effect of Droplet Volume .................................................................................. 59

4.7 Chapter Conclusion .......................................................................................... 60

5 Conclusions ........................................................................................................... 62

5.1 Summary of Contributions ................................................................................ 62

5.2 Future Works .................................................................................................... 65

References .................................................................................................................... 66

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LIST OF FIGURES

Figure 1: Cross-sectional views of a DMF device is presented for (a) a closed system configuration, and (b) an open system configuration. A closed DMF system configuration constitutes a continuous upper electrode tied to ground and is coated in a hydrophobic material. The open DMF system configuration system is without the top electrode. ...................................................................................................................... 30

Figure 2: Hardware design of an integrated DMF device is presented. (a) The block diagram of the DMF device comprises of three hardware components, being: (1) the PCB housing firmware and electrodes, (2) personal computer running the control application, (3) a high voltage supply. (b) The modular PCB design using physically separated boards for control logic and electrodes connected by ribbon cables. (c) Photograph of the fully assembled DMF device. ........................................................... 33

Figure 3: Graphical user interface of the DMF device is presented featuring real-time control of 60 electrodes. Buttons and switches provide the capacity to automate recorded sequences and enable AC-like PFM actuation............................................... 34

Figure 4: Droplet velocity versus voltage in a closed configuration is presented for both (a) PDMS and (b) parafilm dielectric layers using water. The mean velocity (circle) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of DC voltage. The closed microfluidic system is configured having 240 micron spacing between top and bottom planes for a fixed droplet volume of 4.2 µL. .. 37

Figure 5: Droplet velocity versus actuation frequency in a closed configuration is presented for both (a) PDMS and (b) parafilm dielectric layers using water. The mean velocity (circle) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of frequency. The closed microfluidic system is configured having 240 micron spacing between top and bottom planes for a fixed droplet volume of 4.2 µL and a 280 V actuation potential. ............................................ 38

Figure 6: Droplet velocity versus voltage in an open configuration is presented, as a comparison between milk (red) and water (blue), for both (a) PDMS and (b) parafilm dielectric layers. The mean velocity (circle/square) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of DC voltage. The open microfluidic system performance is characterised for a fixed droplet volume of 9.0 µL. ........................................................................................................... 40

Figure 7: Milk droplet actuation in open configuration DMF device is presented with parafilm dielectric layer and silicone oil. Electrode pitch is 2.75 mm, droplet volume is 9.0 µL, actuation voltage is 280 V. ................................................................................ 42

Figure 8: Droplet velocity versus actuation frequency in an open configuration is presented, as a comparison between milk (red) and water (blue), for both (a) PDMS and

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(b) parafilm dielectric layers. The mean velocity (circle/square) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of frequency. The open microfluidic system performance is characterised for a fixed droplet volume of 9.0 µL and a 280 V actuation potential. ............................................ 43

Figure 9: Schematic of the LIA fluorescence spectroscopy experiment. An LED, sample droplet, optical filter and photodiode are aligned in the vertical plane. The LED is driven by square wave from a function generator. TTL output from the function generator is given as reference signal to the LIA. Output current from the photodiode is the raw input to the LIA. ...................................................................................................................... 55

Figure 10: Lock-in amplified photocurrent against rhodamine B concentration in 5.0 µL aqueous droplets. The mean photocurrent and corresponding standard deviation of n = 3 repeated measurements are shown as a function of rhodamine B concentration. ..... 56

Figure 11: Lock-in amplified photocurrent against ciprofloxacin concentration in 5.0 µL milk droplets. The mean photocurrent and corresponding standard deviation of n = 5 repeated measurements are shown as a function of ciprofloxacin concentration. ........ 58

Figure 12: Lock-in amplified photocurrent against ciprofloxacin concentration in milk droplets of volumes: (a) 7 µL, (b) 9 µL, (c) 11 µL and (d) 13 µL. The mean photocurrents and corresponding standard deviations of n = 3 repeated measurements are shown as a function of ciprofloxacin concentration. ...................................................................... 60

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1 Introduction

This thesis demonstrates the fundamental functionalities of actuation and detection

required to produce a digital (droplet-based) microfluidic device for dairy testing.

This introductory chapter details the motivation for developing a digital microfluidic

dairy tester and states the scope of this work.

1.1 Background

In the interest of public health, the concentration of antibiotic residues in

consumable milk is strictly regulated [1]. In Canada, having antibiotic contaminated milk

arrive at a dairy processing plant yields severe consequences for the offending

producer [2]. The milk arrives at processing plants in common loads transporting

several bulk tanks from multiple producers [3]. If any bulk tank fails antibiotic screening,

the full volume is dumped and the offending producer bears the full penalty [4].

Moreover, a producer whose milk tests positive twice within a 12-month period is

indefinitely suspended from the milk market [4]. In the 12-month period ending October

2019, 30 penalties were assessed to dairy producers in Ontario due to antibiotic

contamination resulting in millions of dollars in economic loss [3].

Dairy farmers face an urgent need for development of an on-site sensor capable of

measuring antibiotic concentration within the approximate 5 minutes that each cow is

milked. The common practice of testing the milk after collection in a bulk tank is

inadequate because a single cow’s contaminated milk is sufficient to render the full tank

unusable [5]. Current commercially available on-site tests such as the Delvotest T (DSM

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Food Specialties, Netherlands) and Charm ROSA test (Charm Sciences Incorporated,

United States) are unsuitable for use during the milk collection process due to long test

times [6], [7] and manual procedures [8]–[10].

A potential solution to on-site antibiotic testing is offered by microfluidics.

Microfluidic systems represent the miniaturization of analytical chemistry processes

onto a device with micron-scale features. Miniaturization of chemical processes yields

advantages including portability, minimal reagent consumption and fast response time

[11]–[13].

A subset of microfluidics known as digital microfluidics (DMF) specializes in highly

scalable, automatable and parallel operations [14], [15]. A DMF chip uses a grid of small

electrodes to handle discrete droplets of sample [16]–[18]. Using this technology,

multiple chemical analyses processes can be automated and reconfigured on a single

device. Thus, the capability for automation and versatility of DMF devices makes them

an attractive potential solution to on-site dairy testing.

The application of digital microfluidics to dairy testing is immediately faced with two

fundamental challenges: (1) biofouling and (2) antibiotic detection in droplets. Biofouling

refers to the adherence of fat and protein molecules to hydrophobic surfaces on the

device [19]. Biofouling causes irreversible damage to the device surface and is a

significant issue in microfluidics applications concerning biological samples [14], [20],

[21]. To handle milk droplets along with their fat and protein constituents, a DMF

solution to on-site dairy testing must overcome biofouling. The second fundamental

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challenge for a DMF dairy tester is to detect antibiotic concentrations in milk droplets.

By comparison to traditional microfluidics, DMF is very limited in its ability to separate a

droplet into constituent particles. Thus, a method must be developed to detect antibiotic

contaminants within the bulk droplet. The research presented in this thesis addresses

these two fundamental challenges in actuation and detection to enable future

development of an integrated DMF solution to on-site dairy testing.

1.2 Thesis Scope

The contents of this thesis are described here. Chapter 2 will present a literature

review on the current techniques for antibiotic detection used in off-site laboratories and

on-site at the dairy farm. This chapter also provides background about droplet actuation

on digital microfluidic devices, and will include a review of relevant detection techniques

which have been implemented on digital microfluidic devices.

Chapter 3 presents a fully integrated digital microfluidic device which

demonstrates milk droplet actuation. The design considerations to overcome biofouling

and provide reconfigurability are reported.

Chapter 4 demonstrates a label-free method using fluorescence spectroscopy and

lock-in detection for antibiotic sensing in droplets. The ability to detect antibiotic

concentration in the droplet without need for separation from the bulk medium is well-

suited to digital microfluidic devices.

Chapter 5 reviews the main contributions of this thesis. It also speculates on

important future research.

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2 Literature Review

2.1 Introduction

This chapter is a literature review which will begin by detailing common antibiotic

contaminants regulated in the dairy industry. The methods used to detect these

antibiotics in the lab and on-site will be discussed. Specifically, the advantages and

limitations of traditional microfluidic dairy testers will be discussed. DMF technology is

then detailed with attention to droplet actuation and compatible detection methods.

2.2 Regulated Antibiotics in Dairy

The use of antibiotics to treat livestock has been practiced for decades to promote

health and growth of farm animals [5], [22]. There is strong evidence that the quantity of

antimicrobials used worldwide to treat farm animals is up to four times greater than the

quantity used in human treatment [23], [24]. When these antibiotics are used in food

producing animals, such as cattle, measures must be taken to prevent residues from

appearing in food products.

The presence of antibiotic contaminants in food can have adverse health effects

on human consumers including chemical poisoning, allergic reactions and development

of antimicrobial resistance [25], [26]. It is for this reason that the concentration of

antibiotic residues allowed in consumable milk is regulated in many countries around

the world [5], [27], [28]. In Canada, there exist 96 maximum residue limits (MRLs)

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enforced in the animal food products industry; 36 of these MRLs pertain to milk from

cattle [29].

Antibiotics from four families known as tetracyclines, sulfonamides, β-lactams and

fluoroquinolones are often used in combination for treatment of disease in dairy cows

[24]. The ciprofloxacin antibiotic used in Chapter 4 of this thesis is from the

fluoroquinolones family.

2.3 Laboratory Detection Methods

Since the first reported detection of antibiotics in milk in 1965 [22], there has been

exponential growth in the number of publications related to antibiotic detection in milk

each decade [5]. High pressure liquid chromatography (HPLC) and immunoassays

account for the majority of published research in this field [5]; both methods will be

detailed in this section.

2.3.1 High Pressure Liquid Chromatography

High pressure liquid chromatography (HPLC) is a method of molecular

separation. This technique uses a thin column which is filled with some absorbent

material referred to as the stationary phase [30]–[32]. Outside the column, the sample to

be detected is mixed into a liquid solvent known as the mobile phase [30]–[32]. The

substances used as the stationary and mobile phases are selected with consideration to

chemical properties of the target analyte(s) [30]–[34]. The liquid solution is then pushed

through the thin column under high pressure typically generated by a pump [33]–[36].

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The constituents of the mobile phase will pass through the column at different speeds

depending on their interaction with the stationary phase. This is to say, the greater a

particle’s attraction to the stationary phase, the longer it will take to pass through the

column. Hence, the HPLC column acts as a filter to separate the sample.

It is important to note that HPLC only accomplishes separation. This system is

coupled with some detection method to read concentration of the separated analyte.

Methods including UV-Vis fluorescence [34], [36]–[40] and mass spectrometry [31]–[33],

[35], [41]–[43] have been demonstrated for HPLC coupled antibiotic detection. Using

either of these methods with HPLC separation will allow a time-resolved signal to be

generated. If separation is correctly achieved, signal peaks corresponding to

constituents of the sample will appear after a repeatable duration of time [31]–[40].

Among published works on antibiotic detection in milk, HPLC has been the most

frequently used method [5]. Using HPLC, studies have achieved antibiotic limits of

detection meeting or exceeding regulatory limits [31]–[40].

The limitations of HPLC with respect to on-site antibiotic testing are the need for

bulky lab equipment, extensive sample preparation and the relatively slow response

time. Even under high pressures up to 50 MPa, the fastest antibiotic tests with HPLC

take about 10 minutes [33]. This excludes time needed for centrifuging the sample and

mixing analytes into the mobile phase solution. Hence, HPLC is the golden standard of

antibiotic testing in the lab but has inherent limitations which do not make it adaptable

for on-site testing.

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2.3.2 Immunoassays

The immunological approach to antibiotic detection takes advantage of the highly

selective binding that occurs between antigens and antibodies produced by animal

immune systems [44]. In animal immune systems, the antigen is a compound which

incites an immune response [44]. An antibody is a protein produced by the immune

system to combat a specific antigen [44]. Likewise, an antibiotic is a synthetically made

compound to combat an antigen [44], [45]. An immunoassay for antibiotic sensing uses

the corresponding antigen to label the target antibiotic [44], [45].

An immunoassay is carried out in a well plate. To prepare the well plate, the well

surfaces must first be coated with the antigen or antibiotic that will bind to the target

analyte. For antibiotic testing, the well plates are typically coated with the required

antigen [46], [47]. The antigen free sites on the well-plate are coated with a blocking

protein [47]–[49].

To allow for optical detection after the immunological binding, a fluorescent or

coloured molecule is also conjugated with the antigen or to a secondary antibody [10],

[44], [45], [47]. Commonly used fluorescent labels for antibiotic detection include

horseradish peroxidase, gold nanoparticles, and in more recent work, quantum dots

[10], [46], [47]. Quantum dots are synthetic semiconductor nanoparticles that can be

manufactured to fluoresce at different wavelengths when stimulated with UV light. The

versatile optical behavior of quantum dots makes them well suited to multiple antibiotic

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detecting immunoassays where each antigen can be conjugated with its own coloured

quantum dot [10], [47].

When the well plate surfaces have been prepared, the sample solutions are

dispensed into the well plates. Typically, a 96-well plate is used and immunoassay tests

can be run in duplicate or triplicate [49]. The sample solutions must often be incubated

in the wells at constrained temperature conditions [6], [7], [44], [50].

The completed immunoassay is typically washed with a buffer solution which

removes any unbound antigens from the surface [44], [45]. To read the concentration of

antibiotics, each micro-well in the well plate is interrogated by fluorescence or

absorbance spectroscopy [10], [47], [51], [52]. Comparing to blank samples and known

concentrations included in the immunoassay, the antibiotic concentrations are

determined.

Immunoassays show excellent selectivity and versatility for antibiotic detection.

One study by Song et al. used quantum dot fluorescent labels to achieve simultaneous

detection of three antibiotic families in milk samples and achieved a 5 ppb limit of

detection [47]. However, the immunoassay took a 1 hour incubation time in addition to

the preparation time. Another work showed a rapid immunoassay coupled with

chromatography separation to get concentrations of 27 antibiotics in approximately 20

minutes [10]. In summary, the immunoassay is a scalable and accurate analysis method

but its dependence on label molecules and extensive preparation process make it

impractical to implement outside a traditional laboratory.

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2.4 On-site Detection Methods

This section details methods for dairy testing which have demonstrated the

portability to be used on-site. The limitations in automation, scalability, response time,

and robustness which prevent these methods from being used during milk collection are

discussed.

2.4.1 Lateral Flow Assay

The lateral flow assay is a type of immunoassay analysis which uses capillary

forces to pull the sample fluid across a test strip [53]. At specified lengths, the test strip

is lined with antigens which will selectively bind to their target antibody [9], [50], [51],

[53]–[56]. Thus, the target antibody binds to the labelled antigen and the newly formed

conjugate is carried the length of the strip [9], [50], [51], [53]–[56]. By measuring the

intensity of colour produced at the detection end of the strip, the concentration of the

conjugate and therefore the antibiotic can be quantified [9], [50], [51], [53]–[56].

Research studies have shown the capability of lateral flow assay sensors to

detect up to five antibiotics on a single strip [54]. This is accomplished by creating

multiple reaction zones on the strip where the surface of each zone is functionalized

with the complementary antigen for the targeted antibiotic [54]. The antigen-antibody

conjugates which form continue down the chip and travel through multiple reaction

zones which selectively immobilize the conjugates [9], [51], [53]–[55]. The final result on

the strip is multiple lines appearing near the detection end; the colour intensity of each

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line can be read by a spectrometer to identify concentration of the specified antibiotic

[9], [51], [53]–[55].

Lateral flow assays have demonstrated the ability to detect antibiotics from the

four major antibiotic families of beta-lactams, tetracyclines, sulfonamides and

fluoroquinolones [51], [56]. Furthermore, limits of detection on the scale of 0.1 – 10 ppb

have been achieved [51], [53], [54], [56].

The fastest lateral flow assay test time reported in literature was found to be five

minutes [53]. However, this does not account for the time the milk sample had to be

centrifuged prior to testing or the time for optical testing required after the assay.

The lateral flow assay has been used in commercial products for on-site

antibiotic testing. Examples of such products are the Charm ROSA Test and BetaStar

Plus Test (Neogen, United States). These tests have been studied to perform with

strong specificity and accuracy to detect beta-lactam and tetracyclines below their

MRLs [9], [55]. Moreover, some of the Charm ROSA Tests show a relatively fast

response time of 8 minutes [9].

Although lateral flow assays show strong portability, sensitivity and specificity,

there are limitations in their design that prevent their adaption for use during the milk

collection process. For most antibiotics, the test is advertised to take between 8 – 15

minutes which is beyond the approximate 5 minute period it takes to milk a cow [57].

Reading the test strip often requires trained personnel [9]. Also, the manual

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implementation and single use nature of the technology make it expensive and

challenging to automate.

2.4.2 Prepared Incubated Test

The prepared incubated test uses a colourimetric chemical reaction to indicate the

presence of antibiotics in a milk sample [6], [7]. An example of a commercial product

using this method for on-site antibiotic testing is the DelvoTest T. This product provides

farmers with an incubated well-plate holding small vials of the reactive solution which

appear purple in colour. The user adds 100 µL of raw milk to the vial and allows the

incubator to set for three hours at 64 ºC. After this time, the solution will turn to a green

colour if antibiotic residues are present. A sample without residues will remain purple.

The results of the incubated test are meant to be visually interpreted as positive or

negative depending on colour of the solution. However, a study has shown that

spectroscopic analysis of the sample can be used to quantify concentration of

antibiotics [6]. It should be noted that such analysis can only give an idea of general

antibiotic concentration in the milk but does not indicate concentration of any specific

antibiotics [7].

To characterize accuracy of the DelvoTest, an experiment has been conducted to

test 27 antibiotic residues in raw milk [7]. The researchers found that the DelvoTest

consistently detected 23 out of the 27 antibiotics when they were present at levels

exceeding the MRL mandated by the European Union. The remaining 4 antibiotics had

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a false-negative rate between 1.7% and 4.9%. The DelvoTest has been reported in

other studies to be unreliable for detection of tetracycline antibiotics [6], [7].

The advantage of the prepared incubated test is that there is no preprocessing of

the milk required. The readings also show accuracy suitable for on-site testing and

multiple antibiotics can be tested simultaneously. However, the test requires hours to

complete. There is also responsibility of the user to maintain the temperature of the

incubation and read the final output. These limitations make the method infeasible for

an automated, high throughput dairy sensor.

2.4.3 Microchip Capillary Electrophoresis

A more recent advancement to dairy testing has been the application of

continuous flow microfluidics. These continuous flow microfluidic devices leverage an

actuation technique termed microchip capillary electrophoresis (MCE) [37]–[40], [42],

[43], [58]–[61]. MCE uses the interaction between actuation forces of electroosmotic

flow and electrophoresis to achieve milk sample separation [58].

An MCE device features fluid channels that are microns wide and usually

centimeters long to transport the sample solution. Electrodes are placed at the ends of

the fluid channel so that voltage can be applied [59]. The walls of the microfluidic

channels are made from borosilicate glass, polydimethylsiloxane (PDMS) or a similar

material. It is important that the material of the channels should become deprotonated

by contact with aqueous electrolyte solution and therefore take a negative charge [62].

This deprotonation is required to enable electroosmotic flow [62], [63].

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The electroosmotic flow is the dominant driving force in MCE. The electroosmotic

flow results from the interaction between the negatively charged channel surface, polar

aqueous solution and external electric field [63]. Firstly, the negatively charged channel

surface causes the polar aqueous molecules to adhere to them. Thus, what is known as

the electric double layer is formed by the channel walls and water molecules [64]. When

an external DC voltage is applied across the fluid channel, a uniform electric field is

created [59]. Within this electric field, the negative charges on the channel walls will

migrate towards the cathode at an approximately constant velocity [64]. Subsequently,

the electric double layer mobilizes toward the cathode. Because the channels are only

microns wide, viscous effects in the fluid are sufficient to pull the bulk solution towards

the cathode [62]. By this mechanism, electroosmosis creates an approximately constant

fluid velocity towards the cathode.

The separation of constituents in the sample solution is achieved by

electrophoresis. The electrophoretic force acting on a particle is the force induced on a

particle by an external electric field [64]. The velocity of a particle due to electrophoresis

is proportional to its charge and size [65]. This is to say, charges with different charge

and mass properties will move at different velocities in an electric field.

In MCE applications, the electroosmotic force acting on the sample solution will

cause a net flow towards the cathode. Simultaneously, the electrophoretic force acting

on each particle will result in varied force of attraction to the cathode or anode. The

cumulative result is the net flow of fluid towards the cathode while constituents of the

fluid spread apart due to electrophoresis [62], [64], [65].

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Once separated, the fluid constituents can be detected. MCE devices have

successfully been coupled with fluorescent labels [66], electrochemical sensors [65],

UV-Vis fluorescence spectroscopy [37], [38], [40], [58], [60], [61] and mass spectrometry

[41]–[43], [61] to measure concentration of antibiotics in milk. MCE has strength in

sensitivity as several of these previous works demonstrated limits of detection

exceeding regulatory limits [37]–[43], [60], [61], [66]. However, MCE faces significant

challenges in robustness and automation.

The narrow channels in continuous flow microfluidic are extremely prone to

becoming clogged by fat and protein biomolecules. For this reason, MCE applications

using milk must centrifuge or filter the milk before loading onto the device [37], [38],

[40]–[43], [58], [60], [61], [67]. The channels must also be thoroughly rinsed with custom

buffer solutions between each trial [37], [38], [40]–[43], [58], [60], [61], [67]. This

requirement for preprocessing and manual rinsing requires equipment and time that is

unavailable during an on-site milk collection process.

Additionally, MCE dairy applications typically require voltages in the range of 14

kV – 30 kV [37], [38], [40]–[43], [60], [61], [67]. Although one previous work by Bosma et

al. reduced the voltage level to 500 V, sacrifices were made in response time (18

minutes) and limit of detection [58]. These voltage levels may be challenging to

generate in an on-site device with respect to miniaturization and safety.

In summary, traditional microfluidic devices have demonstrated the portability and

sensitivity for dairy testing. However, the need for milk sample preprocessing, time

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consuming manual rinsing and particularly high voltage requirements make MCE

unviable as an on-site dairy tester.

2.5 Actuation on Digital Microfluidic Devices

This section provides background on the design and actuation of droplets on a

digital microfluidic device.

2.5.1 General Digital Microfluidic Design

A DMF device uses a grid of isolated electrodes to transport droplets of sample

fluid in two dimensions. The electrodes typically have length and width on the scale of

millimeters and can be patterned in a variety of geometries [68]. These electrodes are

used to generate localized electric fields which drive the movement of liquid droplets. As

such, each electrode must have a switchable connection to ground and voltage high. An

insulating dielectric layer is coated over top the electrodes. It is common for digital

microfluidic devices to use voltages up to 400 V [69] and so the dielectric layer is

needed to prevent arcing between electrodes. A hydrophobic layer is then coated over

the dielectric to minimize adhesion to the droplet. This hydrophobic layer eases droplet

movement over the electrodes.

There are two main actuation forces used to drive droplet movement:

dielectrophoresis and electrowetting-on-dielectric (EWOD) [14]. Dielectrophoresis

applies a non-uniform dielectric field to drive movement of a polarizable liquid [70], [71].

The direction of movement of a droplet under dielectrophoresis is dependent on how

polarizable the droplet is relative to the surrounding medium [72]. If the droplet has

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greater dielectric constant than the filler medium, it is pulled towards the cathode [71]. A

droplet with dielectric constant less than the filler medium will be pulled towards the

anode [71]. Dielectrophoresis is used to handle insulating droplets such as deionized

water [71] and oils [70], [72]–[74].

EWOD is the more common actuation force in DMF applications [14], [15].

EWOD applies an external electric field to drive movement of a conductive liquid [16],

[17], [73], [74]. Most reported DMF applications use conductive aqueous droplets and

thus, EWOD is more commonly used [14]. The presence of the electric field causes

polarization of the dielectric layer and droplet. Consequently, an electric double layer

develops between the dielectric and droplet which causes an increased attraction over

the polarized surface [16]. Using this EWOD effect, the droplet is pulled in the direction

of the electric field. Further detail on EWOD and design of an EWOD driven DMF device

is given in Chapter 3.

2.5.2 Biofouling

Biofouling is an important effect to consider in DMF devices working with food

sample droplets such as milk. Biofouling refers to the effect of biomolecules including

fats and proteins adhering to the surfaces of the DMF devices [19], [21]. Even

hydrophobic coatings are prone to biofouling when they come in contact with

biomolecules [75]. For DMF devices, droplet actuation depends on a homogenous

hydrophobic coating across the device surface. By irreversibly contaminating the device

surface, biofouling causes droplets to become stuck at the site of fouling thereby

disabling droplet actuation [21].

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One previous work mitigated biofouling by adjusting the sample solution pH,

using AC voltage actuation and limit the time that voltage is applied [76]. However, this

requires manual preparation of the reagent solution and does not allow the droplet to sit

stationary as would be required for any detection measurements.

Another work addresses biofouling in EWOD with etched nanostructures on the

device surface [77]. This approach has the disadvantage of complex and expensive

device fabrication.

The most common solution to biofouling has been the use silicone oil filler

mediums [15], [78], [79]. This approach surrounds droplets with low viscosity silicone oil

which encapsulates droplets and prevents physical contact with the device surfaces.

The disadvantages of using a silicone oil filler medium are discussed in the following

section.

2.5.3 Filler Medium

As described above, DMF is performed with droplets positioned above a grid of

electrodes. Thus, the droplets are surrounded by a fluid filler medium. The requirements

of the filler medium to facilitate droplet movement are low viscosity, electrically

insulating and immiscibility with the sample droplet [15]. The two most commonly used

filler mediums are air and low viscosity silicone oil [15].

The motivations for using a silicone oil filler medium are lowered actuation

voltages [80], faster droplet speeds [17] and reduced physical contact between the

droplet and solid surfaces [15]. The reduced physical contact is used in applications

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where biofouling is a concern. Using a silicone oil filler medium, DMF devices have

been demonstrated to handle bio-fluids including human blood and saliva [78].

However, the use of an oil filler medium comes with the problem of emulsification and

interference with the sample droplets [11], [15], [74], [78]. To mitigate an oil filler

medium’s interference with sample droplets, chemical modifications to the sample

solution are needed [15]. Hence, the use of an air filler medium is preferred for

applications where accurate chemical analyses of the sample are valued.

2.6 Detection on Digital Microfluidic Devices

To adapt digital microfluidics for dairy testing, a method to detect antibiotic

residues in milk droplets must be determined. In this section, the available chemical

detection methods which have been previously integrated with digital microfluidic

devices are described.

2.6.1 Fluorescence Spectroscopy

Fluorescence spectroscopy is an optical detection technique that relies on

exciting a molecule by exposure to electromagnetic radiation and subsequently

measuring the lower-energy electromagnetic radiation emitted by the molecule [81].

This molecule, known as a fluorophore, absorbs the initial light and an electron is

elevated to a higher energy state [81]. The electron then falls to a lower energy without

emitting any light through a process termed internal conversion [81]. Finally, the

electron returns to its ground state and emits light at a wavelength proportional to the

difference in energy levels [82].

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The energy level of the incident light used to excite the molecule and energy

level of the emitted light are dependent on the chemical properties of the molecule [82].

This is to say, the wavelength used for excitation and emitted wavelength are

dependent on the target analyte. Additionally, in cases where the fluorescence

characteristics of the target analyte are undesirable, a fluorescent label can be used. A

fluorescent label is a molecule which binds to the target analyte and has a known

fluorescent response [10], [47]. Thus, applying fluorescence spectroscopy to measure

concentration of the label is analogous to directly measuring concentration of the

analyte it binds to.

Optical detection techniques such as fluorescence spectroscopy are well suited

to microfluidic devices due to the small footprint of optoelectronics and the ability of light

to travel in small spaces. Moreover, the common use of transparent materials in

microfluidic fabrication such as PDMS and indium tin oxide (ITO) make the devices fit

for optical coupling. Using LEDs, photodiodes and optical filters, past works have

produced fully integrated digital microfluidic devices offering fluorescent sensing [83],

[84]. Optical spectroscopy in microfluidics is traditionally performed in the vertical plane

(perpendicular to sample motion). However, some works have used fiber optic cables to

enable fluorescence spectroscopy in the horizontal plane thereby increasing sample

path length and sensitivity [52], [85]. Thus, attractive features for use of fluorescence

spectroscopy with digital microfluidics include minimal space requirement and

compatibility with traditional fabrication methods.

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2.6.2 Surface Plasmon Resonance

Surface plasmon resonance (SPR) is an optical detection technique which

requires a thin reflective surface placed between a prism and a medium with lower

refractive index than the prism [86]. Common configurations use a gold film tens of

microns thick between a prism and an air or solution medium [87]. A beam of polarized

light is shot on the gold surface through the prism and photons meeting the resonant

energy of the surface will be absorbed while other wavelengths are reflected [86], [88].

Using a sensor to capture the reflected light, the resonant wavelength can be identified

as a dark band in the spectrum. SPR leverages this phenomenon by immobilizing

molecules which bind to the target analyte onto the gold surface; when binding occurs

between the immobilized surface molecules and analyte, the resonant energy of the

surface changes [88]. Thus, when the immobilized molecule is correctly selected,

measuring the resonant wavelength as analyte passes over the surface gives time-

resolved concentration data [87].

SPR has been demonstrated in traditional microfluidic systems to detect multiple

antibiotic families in milk with limits of detection below Canadian MRLs [89], [90]. This

method has also been integrated with digital microfluidics [91]. SPR offers strong

sensitivity. Weaknesses include complex and expensive fabrication of the sensor

surface.

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2.6.3 Impedance Spectroscopy

Impedance spectroscopy (IS) is a technique where alternating current (AC) low

voltage signal is applied across the sample while the response is measured in form of

current or impedance [92]. From measuring the magnitude and phase responses as a

function of frequency, the real and imaginary components of the sample’s impedance

are obtained [92]. The real component of impedance represents the resistive element of

the sample while the imaginary component represents the capacitive element [92], [93].

By comparing known IS responses with the signature given by a sample, properties of

the sample such as concentration of an analyte can be inferenced [92]–[94].

Previous work has integrated IS with digital microfluidic [93], as well as traditional

microfluidic systems where the presence of DNA and antibodies were detected with

limits of detection on the nanomolar scale [94]. IS is relatively easy to integrate with

digital microfluidics as it only requires two electrodes able to simultaneously contact the

sample. Disadvantages include the fact that the electrodes usually have a hydrophilic

surface making them prone to biofouling [19], [95].

2.6.4 Electrochemical Detection

Electrochemical detection techniques require three separate electrodes: the

working electrode, reference electrode and counter electrode [96]. The reference

electrode houses a redox reaction independent from the analyte solution in order to

provide a known reference potential [96]. Thus, a potential can be applied or measured

in reference to this known potential. The counter electrode is available as a path for

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current to flow between itself and the working electrode when voltage is applied [96].

Using this three electrode configuration, three main measurement methods can be

used: potentiometry, amperometry and voltammetry.

Potentiometry measures the voltage between the working electrode and reference

electrode while immersed in the sample solution [97]. Amperometry measures the

current through the sample when a known voltage is applied to the working electrode

[97]. Lastly, voltammetry is the most versatile method of the three as it measured

voltage and current [97]. Voltammetry uses a device called a potentiostat to sweep

through a range of voltages applied to the working electrode and measure the resulting

currents in the sample; this generates a plot known as a voltagramm [97]. These

measurements can be performed with or without the use of labels. From each of these

methods, the measured response from a sample can be compared against calibration

data to determine concentration of an analyte [96], [98], [99].

Previous works have used potentiometry and label molecules to detect tetracycline

antibiotics in milk at concentrations low as 1 ppb [100]. Moreover, studies have

integrated the three electrode configuration on digital microfluidic chips and

demonstrated the capacity for potentiometric sensing [96], [98]. A significant drawback

of potentiometric sensing is vulnerability to biofouling due to the hydrophilic electrode

surfaces [19].

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3 An Integrated Digital Microfluidic Device for Dairy Applications

This chapter addresses the problems of overall device integration and milk droplet

actuation for a digital microfluidic dairy testing device.

3.1 Chapter Introduction

The study of microfluidics represents the miniaturization of traditional chemical

analyses processes onto a single integrated device [59], [101]–[103]. Microfluidics offers

advantages in portability, fast response time and minimal reagent consumption over

their full-scale laboratory counterparts [14]. This technology has been adapted to on-site

applications including clinical diagnostics [104], environmental testing [105] and

biological cell culturing [106]. Traditional microfluidic devices transport reagent fluids

through micron-scale width channels driven by hydraulic pressure [66], [107] or electric

field gradients [58]. This method of microfluidics is broadly termed continuous flow

microfluidics.

More recently, a subset of microfluidics known as digital microfluidics (DMF) has

garnered increased favor due to its unique ability to handle samples in discrete droplets

over an array of electrodes rather than through continuous fluidic channels [16]. Where

traditional microfluidic devices are limited in flexibility by the fabrication of rigid fluid

channels, DMF devices offer the potential to be reprogrammed to achieve

reconfigurability, automation and highly parallel operations [108].

The optimal design of an integrated DMF device, having fully leveraged the

aforementioned capabilities, is an on-going effort. As such, there is a need for further

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automation of DMF devices. This is particularly true to on-site applications, such as on-

farm dairy analyses [58], [59].

A significant challenge faced in the microfluidics domain, being relevant to

applications concerning biological samples, is the phenomenon known as biofouling.

Biofouling refers to the adhesion of fat and protein biomolecules to the fluid handling

surface of the microfluidic device, resulting in damage and the degradation of system

performance [19].

In this chapter, we address the issues of overall device integration and biofouling

within a DMF device. An integrated DMF device controlled through a versatile graphical

user interface (GUI) computer program is demonstrated to actuate milk droplets. The

velocities of milk and water droplets are compared for different dielectric coatings and

device configurations to address the effect of biofouling. The results of this chapter are

important in demonstrating an integrated DMF design suited to bio-fluid actuation and

opening the use of DMF devices in dairy testing applications.

3.2 Background

Dairy testing is an important field of research which has seen exponential growth

in published literature over the past several decades [5]. Around the world, veterinary

drugs are administered to dairy cattle to promote growth, control breeding and treat

disease [26], [109]. Consequently, the administered antibiotics and their metabolites are

prone to appearing in the milk produced by these cattle in the form of antibiotic residues

[26]. The presence of antibiotic residues in the dairy milk can be directly toxic to human

consumers [26] or cause the development of unwanted antibiotic resistance [110]. To

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address this problem, worldwide regulatory bodies conduct laboratory tests for

identification of antibiotic residues in dairy products which are made available for

consumption [111].

There is an important need for the development of an on-site dairy tester which

has not been met by existing technology. Traditionally, testing milk for antibiotic

residues occurs at an off-site milk processing laboratory [2]. The farmer is not equipped

to test milk on-site at the dairy farm before bulk tank collection and shipping to the

processing facility [58]. Consequently, the farmer’s dairy enterprise is burdened if

contaminated milk is inadvertently collected. By submitting non-compliant milk to supply

chain stakeholders, the farming enterprise is penalized with monetary fines and loss of

licensure after multiple offences [2]. Modern commercially available methods for on-site

dairy testing are unviable to use during milk collection because of their manual

requirements, long test times and need for trained personnel [7], [9].

A promising move towards on-site dairy testing is offered by microfluidic

technology. Previous studies applying continuous flow microfluidics to dairy testing have

demonstrated the capacity to separate and detect antibiotic residues in milk [37]–[39],

[43], [58], [66], [67], [112]. However, continuous channel microfluidic systems face

significant challenges in robustness and automation which limit their suitability for on-

site dairy testing. To prevent fat and protein molecules in milk from clogging the narrow

channels, the milk samples must be centrifuged or filtered before loading onto the

microfluidic device [37]–[39], [43], [58], [66], [67], [112]. The fluid channels must also be

carefully rinsed for several minutes with custom buffer solutions between each trial [37]–

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[39], [43], [58], [66], [67], [112]. These manual processing steps require time and

equipment which is not available during a dairy farm’s milk collection process.

DMF is an alternate technology which addresses the limitations in robustness

and scalability faced by conventional continuous microfluidics. DMF handles liquid

samples in discrete droplets across an array of addressable electrodes as opposed to in

narrow channels. By applying voltage to the individual electrodes, a dielectric surface is

polarized and attracts droplets of conductive liquid by a force known as electrowetting-

on-dielectric (EWOD) [108]. DMF devices have been demonstrated to transport, split

and mix liquid droplets thereby showing their capacity for lab-on-chip functionality [113].

Scalable designs for droplet actuation [18] and position sensing [103] allow DMF

devices to handle multiple droplets in parallel. Hence, DMF devices offer capability for

automation, reconfiguration and parallel throughput required by an on-site dairy tester.

DMF encounters two challenges in being adapted for dairy testing. These

challenges are as follows: (1) integration of automation and reconfigurability and (2)

overcoming biofouling. A DMF device for dairy testing must feature ease of

reconfiguration and automation to be used for detecting multiple antibiotic residues in an

on-site solution. The device also has to overcome biofouling to prevent biomolecules in

milk from adhering to the chip surface and causing the droplets to become immovable

[21].

Important previous works reporting integrated DMF devices are the DropBot by

the Wheeler Microfluidics Laboratory [12] and the OpenDrop by Gaudi Labs [11]. The

DropBot is a DMF fixture which allows droplet position sensing, instantaneous droplet

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velocity measurements and droplet actuation. The DropBot is an excellent research tool

but requires a complex and bulky assembly not suitable to on-site applications. By

contrast, the OpenDrop is a simpler DMF assembly which uses via-hole routing to

construct a densely packed array of electrodes. Users control the droplet position

through a button and joystick interface. The drawback of this embedded user interface

is that complex functions such as multiple droplet handling and automation are non-

intuitive and challenging to achieve for the user.

In this work, we address DMF integration challenges as we have built an

integrated and modular printed circuit board (PCB) design allowing individual control of

60 electrodes connected by through-hole via routes. The electrodes are controlled

through a user-friendly GUI application which allows real-time electrode switching and

automation through recorded sequences. Thus, parallel handling of multiple droplets

and automation are easily achieved and reconfigured.

To address the issue of biofouling, we develop a novel DMF chip with enhanced

properties of a silicone oil hydrophobic layer. The velocity of milk droplets is quantified

in relation to water when device configuration and dielectric coating material are varied.

The actuation of milk droplets is demonstrated within an air filler medium as opposed to

an oil filler medium. Oil filler mediums reduce the voltage needed for droplet actuation

[80], however, they require more complex device fabrication and interfere with biological

samples [11], [15]. For this reason, silicone oil was used only as a hydrophobic layer

while the droplets were surrounded by air. The velocity of milk and water droplets were

measured in closed and open DMF system configurations. The closed DMF system is

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differentiated by presence of a top electrode which sandwiches the droplet. The effect of

dielectric material on biofouling was also studied by measuring droplet velocity when a

gel-based polydimethylsiloxane (PDMS) or thin-film parafilm dielectric were used in the

DMF device.

3.3 Electrowetting Actuation

The EWOD effect used to actuate droplets in a DMF system is based on the

manipulation of surface energy at the interface between a polarizable solid layer and a

conductive liquid droplet [16]. The Lippmann equation expresses this relationship as

𝛾𝑆𝐿(𝑉) = 𝛾𝑆𝐿(0) −휀𝑉2

2𝑑 ,

(1)

where 휀 and 𝑑 are the permittivity and thickness of the solid layer respectively, 𝑉 is the

potential applied across the dielectric layer, 𝛾𝑆𝐿(0) is the solid-liquid surface tension at

rest and 𝛾𝑆𝐿(𝑉) is the solid-liquid surface tension in the presence of an electric field

applied across the dielectric. The Lippmann equation is complemented by Young’s

equation which relates the surface tensions at a three phase solid-liquid-gas interface

as

𝑐𝑜𝑠𝜃𝐶 =𝛾𝑆𝐿 − 𝛾𝑆𝐺

𝛾𝐿𝐺 , (2)

where 𝛾𝑆𝐺 and 𝛾𝐿𝐺 are surface tensions at the solid-gas and liquid-gas interfaces

respectively and 𝜃𝐶 is the contact angle formed between the surface and inner edge of

the liquid as labelled in Figure 1. By substituting (1) into (2), the resulting Young-

Lippmann equation shows

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𝑐𝑜𝑠𝜃𝑉 = 𝑐𝑜𝑠𝜃0 +휀𝑉2

2𝛾𝐿𝐺𝑑 ,

(3)

where 𝑐𝑜𝑠𝜃0 and 𝑐𝑜𝑠𝜃𝑉 represent the solid-liquid contact angle at rest and in the

presence of an electric field.

The Young-Lippmann equation shows that the contact angle at a dielectric solid-

liquid interface decreases when an electric field is applied; this phenomenon is known

as EWOD. In DMF devices, EWOD is leveraged by switching localized electric fields to

create an unbalanced interfacial tension across a liquid droplet [16]. The resulting

pressure gradient across the droplet causes it to translate in the direction of the

activated electrode [113].

Although actuation of aqueous droplets has been repeated across many works,

handling milk samples is more complex. This is due to the biofouling effect which

causes the device’s surface to be irreversibly contaminated by fats and proteins [19].

Additional opposing forces to EWOD include surface roughness and contact angle

hysteresis [114]. In this chapter, we overcome these opposing forces to demonstrate

milk droplet actuation.

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Figure 1: Cross-sectional views of a DMF device is presented for (a) a closed system configuration, and (b) an open system configuration. A closed DMF system configuration constitutes a continuous upper electrode tied to ground and is coated in a hydrophobic material. The open DMF system configuration system is without the top electrode.

3.4 General DMF Design

General design of a DMF system includes the material layers shown in Figure 1.

The bottom layer is composed of isolated electrodes which should always be pulled low

to ground or high to the supply voltage. A dielectric layer over electrodes provides the

high impedance needed to prevent leakage currents between alternately switched

electrodes and create the electric field gradient needed for EWOD. The dielectric layer

also serves as the polarizable solid surface for EWOD. A hydrophobic coating is used to

reduce surface forces and ease droplet translation. Note from Figure 1 that the droplet

volume must be large enough that the droplet overlaps with adjacent electrodes. This

arrangement is necessary to facilitate actuation by EWOD [17].

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DMF devices can be designed in closed and open configurations as pictured in

Figure 1(a) and Figure 1(b) respectively. By contrast to an open configuration, the

closed configuration uses a continuous top electrode to sandwich the droplet with the

bottom layer. The closed configuration allows smaller droplet volumes than an open

configuration as the sandwiched droplet more readily spreads onto adjacent electrodes.

Moreover, the presence of the top electrode creates a strong vertical component of the

electric field gradient. This arrangement allows improved control and alignment of

droplets over the activated electrodes when compared to the open configuration [17]. To

perform more complex operations of droplet splitting and dispensing, a closed

configuration is needed [115]. In the open configuration, frictional force between the

droplet and top layer is eliminated. The open configuration is also advantageous in

providing access to the droplet for sensors [116] and for handling larger volume

droplets. The device demonstrated in this work can be operated in both closed and

open configurations.

The choice of material and thickness of the dielectric layer are also important

parameters which affect droplet mobility in a DMF system. As given by equation (3), a

thinner dielectric layer results in a greater change of contact angle during EWOD.

Simultaneously, the dielectric must have sufficient dielectric strength and thickness to

withstand the applied voltages without breaking down. Previous works have shown

dependence of droplet velocity on dielectric thickness and material [103].

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To experimentally determine the effect of DMF device configuration and dielectric

material on biofouling, an easily modifiable DMF design was required. We address this

need with a modular integrated DMF design detailed in the following section.

3.5 DMF Prototype Design

The DMF device PCB pictured in Figure 2(b) was divided into two separate

boards: the electrode board and the control board. The electrode board incorporated 60

interdigitated electrodes of varied pitch and spacing. For our experiments, a 6 by 6

electrode grid of 2.75 mm dimensioned square electrodes with 100 micron spacing was

used. The electrode board featured four-layers and via-holes to reach each of the

individually addressable electrodes. Creepage and clearance between routes was

managed to safely accommodate up to 300 V in adherence with IPC-2221 guidelines

when a conformal coat was applied [117]. The physical separation of the electrode

board from the control board allowed experimenting with electrode surface treatments

without consequence to the control electronics.

The control board architecture incorporated an Arduino Nano microcontroller

running a finite state machine firmware. This event driven firmware was responsible for

receiving commands from the GUI application and relaying signals to an HV507 serial-

to-parallel converter (Microchip Technologies Inc.). The HV507 is a push-pull high-

voltage driver with 64 channels and rated up to 300 V. Commands from the GUI

application were sent to the microcontroller over a universal asynchronous receiver

transmitter (UART) serial connection. Commands for toggling electrodes on-off were

sent with a 64-bit integer argument where each bit corresponded to the switch status of

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an individual electrode. The microcontroller parsed the 64-bit argument and drove the

corresponding electrode channels through the HV507. At a UART communication rate

of 9600 bits per second and microcontroller clock rate of 16 MHz, this method allowed

switching times less than 15 milliseconds.

Figure 2: Hardware design of an integrated DMF device is presented. (a) The block diagram of the DMF device comprises of three hardware components, being: (1) the PCB housing firmware and electrodes, (2) personal computer running the control application, (3) a high voltage supply. (b) The modular PCB design using physically separated boards for control logic and electrodes connected by ribbon cables. (c) Photograph of the fully assembled DMF device.

The GUI desktop program used to control electrodes and automate sequences is

shown in Figure 3. This application was developed for Windows environments using NI

LabVIEW. From the GUI, users have control and visualization of the actuated

electrodes. Electrodes can be spatially selected via computer peripherals to switch in

real-time or recorded sequences could be played with defined time duration between

steps. The recorded sequences enable easy automated handling of one or many

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droplets simultaneously. An actuation frequency could also be set to drive the

electrodes with an AC-like pulse frequency modulated (PFM) signal with fixed duty cycle

of 50% and user defined frequency. Note that driving a true AC signal would require an

inverter circuit on the PCB.

Figure 3: Graphical user interface of the DMF device is presented featuring real-time control of 60 electrodes. Buttons and switches provide the capacity to automate recorded sequences and enable AC-like PFM actuation.

3.6 Closed Configuration Experiments

The closed configuration experiments were performed with an indium tin oxide

(ITO) top layer as pictured in Figure 2(b). The ITO slide was tied to ground by wrapping

the edges in a copper tape and connecting to a ground wire. The top layer was spaced

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approximately 240 microns apart from the bottom layer by four layers of 60 micron thick

tape. A commercially available fluoropolymer hydrophobic coating called Fluoropel

PFC1601V (Cytonix Inc.) was spin coated onto to the ITO slide.

Closed configuration droplet velocities were calculated using the minimum

electrode switching time required by droplets to travel an automated path. The droplets

were actuated in a square circuit of eight electrodes while the switching time was

reduced until the droplet could not keep pace. Thereby, velocities were calculated using

the electrode pitch of 2.75 mm and the minimum achievable switching time. Beginning

at a voltage of 300 V, the voltage was decremented in steps of 10 V until the droplet

could not be actuated between successive electrodes. Measurements were made in

triplicate at each voltage level with a fixed droplet volume of 4.2 µL.

The droplet velocities versus voltage are plotted in Figure 4 where Figure 4(a)

uses a PDMS dielectric and Figure 4(b) uses a parafilm dielectric. Only water droplet

velocities are plotted in Figure 4 as milk droplets were immoveable in the closed

configuration. The milk droplets left behind residues on the fluoropel coated ITO which

caused droplets to stick to these spots. This biofouling effect could only be corrected by

recoating the ITO with a fresh fluoropel layer. In the closed configuration, milk droplets

could be moved only when the droplet was encapsulated in a silicone oil shell.

Consequences of the silicone oil shell include potential emulsification with the sample

fluid which is detrimental to sensing applications [15]. Our results using an air filler

medium showed that the biofouling effect is dominant in a closed configuration.

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Closed configuration water droplet velocities are plotted against actuation

frequency in Figure 5 with voltage fixed at 280 V. The trend shows droplet velocity is

maximized at DC and decreases to a plateau as frequency is increased. Previous

studies show a similar trend of decreasing EWOD force with actuation frequency [74],

[118], [119]. The complex permittivity of the droplet is given by

휀∗ = 휀 − 𝑗𝜎

2𝜋𝑓 , (4)

where 휀 is dielectric permittivity, 𝜎 is conductivity and 𝑓 is frequency. Equation (4)

shows that the contribution of the droplet’s conductivity to the complex permittivity is

reduced as signal frequency increases [118]. Thus, at high frequencies a conductive

droplet behaves as an insulating droplet. The EWOD force which requires the droplet to

be conductive is then weakened at higher frequencies [15]. The frequency weakened

EWOD force results in a smoother droplet motion which can be leveraged for finer

control over droplet velocity [120].

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Figure 4: Droplet velocity versus voltage in a closed configuration is presented for both (a) PDMS and (b) parafilm dielectric layers using water. The mean velocity (circle) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of DC voltage. The closed microfluidic system is configured having 240 micron spacing between top and bottom planes for a fixed droplet volume of 4.2 µL.

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Figure 5: Droplet velocity versus actuation frequency in a closed configuration is presented for both (a) PDMS and (b) parafilm dielectric layers using water. The mean velocity (circle) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of frequency. The closed microfluidic system is configured having 240 micron spacing between top and bottom planes for a fixed droplet volume of 4.2 µL and a 280 V actuation potential.

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3.7 Open Configuration Experiments

The open configuration eliminates friction between the droplet and the top planar

surface thereby enabling increased droplet velocities when compared to closed

configurations. The weakness of the open configuration is alignment of the droplet over

activated electrodes. Because EWOD is a polarity independent force, there exists a

position of equal electric field gradient exactly in the middle of an electrode at high

potential and an electrode at low potential [17]. Without the vertical field gradient

component given by a top planar electrode, the droplet is prone to becoming “stuck”

between electrodes. There are two solutions for this problem. The first is to increase the

ratio of droplet volume to electrode pitch [17]. The other is to have a densely packed 2D

electrode array whereby the droplet can be recovered when positioned between two

electrodes. In this work, we apply the latter solution using via routing to construct the

electrode array.

Open configuration droplet velocities were measured using video frame analysis

to determine time for the droplet edge to move from one electrode to the center of an

adjacent activated electrode. The droplet volumes were fixed at 9.0 µL. Actuation

voltage was decremented in steps of 10 V until the droplet could not be actuated

between successive electrodes. Figure 6 plots the velocities of water and milk droplets

on PDMS and parafilm dielectric layers respectively. By eliminating droplet contact with

the fluoropolymer hydrophobic layer used in the closed configuration, biofouling of the

fluoropolymer is overcome. The silicone oil layer on the bottom plane forms a thin film

preventing biofouling of the bottom plane.

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Figure 6: Droplet velocity versus voltage in an open configuration is presented, as a comparison between milk (red) and water (blue), for both (a) PDMS and (b) parafilm dielectric layers. The mean velocity (circle/square) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of DC voltage. The open microfluidic system performance is characterised for a fixed droplet volume of 9.0 µL.

From Figure 6 the maximum observed milk droplet velocities were 4.6 mm/s and

8.8 mm/s on the PDMS and parafilm respectively. Similarly, maximum observed water

droplet velocities were 10.9 mm/s and 11.0 mm/s on PDMS and parafilm respectively.

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Milk droplet velocities are significantly less than those of water likely due to the effect of

fat and protein constituents on physical parameters not limited to mass, viscosity and

conductivity. It should be noted that the surface roughness of the PDMS coating had a

significant effect in open configuration experiments. Water and milk droplets on the

PDMS dielectric regularly became stuck between electrodes thereby making continuous

actuation challenging. The PDMS surface roughness was overcome in a closed

configuration due to the improved control of droplet alignment but was a prevalent issue

in the open configuration. By contrast, the parafilm dielectric reliably allowed continuous

actuation of water and milk droplets in an open configuration. To mitigate surface

roughness, more sophisticated coating techniques such as chemical vapour deposition

(CVD) can be used instead of spin coating. Similarly, surface roughness of the PCB

electrodes can be mitigated using the “via in pad plated over” (VIPPO) technique during

fabrication [121].

Snapshots of an automated actuation sequence of a milk droplet are shown in

Figure 7. Droplet velocities at voltages greater than 280 V could not be accurately

measured by the 20 frame per second video camera to be included in Figure 6.

However, open configuration droplet velocities on parafilm of up to 9.2 mm/s for milk

and 27.5 mm/s for water were measured at 300 V by automated actuation of droplets in

a circuit pattern (Figure 7) with minimum switching times of 300 ms and 100 ms

respectively.

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Figure 7: Milk droplet actuation in open configuration DMF device is presented with parafilm dielectric layer and silicone oil. Electrode pitch is 2.75 mm, droplet volume is 9.0 µL, actuation voltage is 280 V.

Open configuration droplet velocities against actuation frequency shown in

Figure 8 give a similar trend to that observed in a closed configuration. As predicted by

equation (4), the EWOD force is maximized at DC actuation for conductive droplets.

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Figure 8: Droplet velocity versus actuation frequency in an open configuration is presented, as a comparison between milk (red) and water (blue), for both (a) PDMS and (b) parafilm dielectric layers. The mean velocity (circle/square) and corresponding standard deviation (vertical bar) of n = 3 repeated measures are shown as a function of frequency. The open microfluidic system performance is characterised for a fixed droplet volume of 9.0 µL and a 280 V actuation potential.

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3.8 Methods

3.8.1 Reagents

5 cSt silicone oil is purchased from Sigma Aldrich (Missouri, United States).

PDMS is purchased from Dow Chemicals (Michigan, United States). Fluoropel 1601V is

purchased from Cytonix LLC (Maryland, United States). Two percent milk is purchased

from a local vendor.

3.8.2 Digital Microfluidic Device Printed Circuit Board

The electrode board and control board were fabricated by JLCPCB (JiaLiChuang

Company Limited, China). The AQW216 solid state replay (Panasonic Corporation,

Japan) provided isolation of high and low voltage. The HV507 serial to parallel high

voltage driver was used to switch voltages to the 60 electrodes. The Arduino Nano

microcontroller firmware was a customized version of the open-source LINX Toolkit

(National Instruments, United States). The GUI control program was built using

LabVIEW 2017 (National Instruments, United States). The PCB was coated in 419D

acrylic conformal coating (M.G. Chemicals, Canada) to meet electrical spacing

requirements up to 300 V given by the IPC-2221 design standard [117]. Conformal

coating was applied by aerosol on the assembled PCB in four coats with four minutes to

air dry between coats. For conformal coat curing, the PCB was left on a hot plate at

80°C for 20 minutes. This process was repeated for both sides of the PCB. The

conformal coat was verified by a wet-gauge comb to have thickness less than 10

microns.

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3.8.3 Dielectric Coating

PDMS coating was applied using the Sylgard 184 silicone elastomer (Dow

Chemicals Company, United States). The PDMS was mixed at a 7:1 ratio of elastomer

to curing agent. The mixed solution was spin coated onto the cleaned electrode PCB at

a maximum speed of 2000 rpm for 20 seconds. Note that conformal coating was not

applied to the electrode boards where PDMS was to be coated. The coated PCB was

left to cure on a hot plate at 105°C for 1 hour and then air cooled until the PDMS was

dry to touch. Two drops of silicone oil (Sigma Aldrich, United States) were applied and

spread gently by gloved finger.

Parafilm coating first required stretching of the parafilm to thin the dielectric layer.

A piece of parafilm was stretched across a flat surface by hand and held in the

stretched position for 10 minutes. The stretched parafilm was secured to a custom 3D

printed carrier by double sided tape. One drop of silicone oil was spread on the

electrode board to prevent air from being trapped between the PCB and parafilm. The

3D carrier was then secured to the electrode board by screws. Two drops of silicone oil

were applied and spread gently by gloved finger.

3.8.4 Statistical Analysis

Measurements of droplet velocity were made in triplicate. The data points plotted

in figures represent the mean of the n = 3 repeated measures. The vertical chart bars

represent distribution of the standard deviation between repeated measures.

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3.9 Chapter Conclusion

In this chapter, an integrated DMF device with a modular PCB design, user-

friendly software interface, reconfigurability and capacity for automation was developed

for bio-fluid handling in an air filler medium. Experiments using closed and open

configurations determined that the open configuration is best suited to mitigate

biofouling due to its removal of physical contact between the sample and the

hydrophobic coating on the top plane. The use of silicone oil on the bottom plane

prevented any biofouling from milk droplets. Comparison of the gel-based PDMS and

thin-film parafilm dielectrics showed that the thin-film dielectrics are advantageous in

reducing surface roughness. Frequency modulation of actuation voltage supported the

understanding that EWOD force is maximized at DC while finer control over droplet

velocity is enabled by AC. Our DMF device demonstrated automated continuous

actuation of milk droplets using an open configuration, parafilm dielectric and silicone oil

coating. Thus, our results demonstrate applicability of DMF to dairy testing by

addressing the fundamental obstacles of device integration and biofouling. These

results respond to an urgent need for an on-site dairy testing technology that provides

robustness and scalability not offered by current methods.

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4 Label-free Antibiotic Detection in Milk Droplets

This chapter addresses the problem of antibiotic detection in milk droplets required

for a digital microfluidic dairy testing device.

4.1 Chapter Introduction

It is a common practice around the world to administer veterinary drugs to cattle

for promoting growth and regulating breeding. Furthermore, antibiotics are routinely

used to treat infections in livestock such as cattle [26], [109]. Consequently, residues of

these antibiotics and their metabolites are prone to appearing in dairy products which

can then have negative health effects on human health including allergic reactions [26]

and antibiotic resistance [110].

To protect public health, regulatory bodies enforce the testing of dairy milk for

antibiotic residues [111]. Dozens of regulated antibiotics must fall under specified

concentration limits in order for the milk to be permissible for human consumption [2].

The tests for antibiotic residues are traditionally performed at a laboratory where dairy

farmers must ship their milk in large containers [58]. The critical flaw in this method is

that dairy farmers are unable to test the milk as they collect it and are therefore

vulnerable to collecting large batches of contaminated milk [58]. Modern commercially

available on-site dairy testing devices have long response times [6], [7] and complex

manual test procedures [9] which make them unviable to use during the milk collection

process. To address this urgent need for an on-site dairy tester, microfluidics represents

a promising research technology.

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Microfluidic devices are miniaturized sensors that aim to replicate chemical

analyses processes performed in a laboratory onto an integrated device; thus, these

devices are often referred to as lab-on-a-chip devices. Advantages of implementing

chemical analyses processes on a microfluidic device include portability, minimal

reagent consumption and high throughput [14], [15]. Traditional microfluidic devices are

based on continuous flow of reagent fluid through micron-wide channels.

In the past two decades, a newer branch of microfluidics known as digital

microfluidics (DMF) has been actively studied [16]. The ability of DMF devices to

transport, split and mix individual droplets of liquid samples across a digitized grid of

electrodes provides a highly scalable lab-on-a-chip architecture [18], [113]. The

reconfigurability of DMF devices yields the potential to perform multiple parallelized

chemical analyses on a single integrated device [122]. DMF devices have found

applications including point-of-care clinical diagnostics [79], [123], environmental testing

[105] and biological cell culturing [106], [124]. In the previous chapter, we overcame

biofouling and presented a fully integrated DMF device for milk droplet actuation.

Hence, the robustness and capacity for automation of DMF devices make them an

appealing option for on-site dairy testing.

For DMF to be adapted for on-site dairy testing, the functionality to detect

antibiotic residues from milk droplets must be demonstrated. Previous works applying

continuous microfluidics to antibiotic detection in milk have used chromatography [38],

[125] and electrophoresis [37], [39]–[41], [58], [60] to separate sample particles based

on mass, charge and chemical structure. The separated particles flow through narrow

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channels on the device for subsequent detection by UV-Vis spectroscopy [37]–[40],

[58], [60] or mass spectrometry [41]–[43], [61]. Although continuous flow devices are

effective in sensing antibiotics, they face significant limitations including need for

preprocessing of milk samples, very high voltages and need for custom buffer solutions

[37]–[43], [60], [61]. To prevent clogging of narrow channels, milk samples must be

centrifuged or filtered using laboratory equipment [37]–[43], [60], [61]. The channels

must then be rinsed for several minutes between each trail [37]–[43], [60], [61]. The

DMF device in the previous chapter is able to actuate milk droplets without any

preprocessing. To achieve fast response times and low detection limits, continuous

microfluidics rely on high voltages in range of 14 kV – 30 kV [37]–[43], [60], [61].

Although voltages low as 500 V have been demonstrated, they sacrifice performance

and sensitivity. These kilovolt scale potentials are challenging to generate in a

miniaturized on-site dairy tester. By contrast, the DMF device in the previous chapter

operates at 280 V which can be reliably produced by a voltage boost converter circuit

[11]. Continuous flow devices also require carefully prepared and stored buffer

solutions to be loaded in the channels for each trial [37]–[43], [58], [60], [61].

To summarize, modern continuous flow devices are unsuitable for on-site dairy

testing due to dependence on laboratory equipment, long preparation times and manual

processes. DMF devices provide valuable improvements in these areas but struggle in

antibiotic separation and detection. In this chapter, we address the functionality of

antibiotic sensing for an on-site DMF dairy tester.

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The most widely used detection method in DMF biosensors is optical detection

including absorbance and fluorescence spectroscopy [15]. Optical detection is well-

suited to DMF devices due to being contact-free, miniaturize-able and accessible. Being

contact-free allows optical detectors to work with biological sample droplets without the

risk of biofouling [19]. Optical equipment including light emitting diodes (LED),

photodiodes and optical filters have the small footprints required to integrate with

microfluidic systems. Compatibility with fiber optic waveguides has further shown

miniaturization of optical detection in DMF devices [103], [126]. Optical detection is also

well-suited to dairy testing as multiple regulated antibiotics are measurable by UV-Vis

spectroscopy [37], [38], [40], [61]. However, without the utility for separation, DMF

sensors commonly rely on label molecules which selectively bind to the target analyte

and are more readily detected [15], [79], [123].

The use of label molecules is undesirable due to cost and complexity. Label

molecules are highly specific and therefore a new label molecule must be used for each

target analyte [45]. As a result, labelled detection of multiple analytes requires multiple

expensive label molecules which are consumed in each trial. The preparation of label

molecules is also commonly customized to each application and requires trained

personnel in a laboratory environment [127]. This dependence on personnel and lab

facilities for label preparation is not well-suited to on-site applications. Thus, the

development of a label-free method of antibiotic detection in DMF devices will be

valuable.

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In this chapter we present a label-free optical detection method for antibiotics in

milk droplets. The presented method is enabled by lock-in amplified fluorescence

spectroscopy. Detection is performed in milk droplets without need for chemical

separation thereby demonstrating compatibility with modern DMF devices. This method

is demonstrated by detection of the ciprofloxacin antibiotic in droplets of milk. The

relationship between droplet volume and fluorescent intensity of ciprofloxacin is also

investigated. The results of this chapter demonstrate a viable detection method for

integration in a DMF dairy tester.

4.2 Lock-In Amplification

The lock-in amplifier (LIA) is a scientific instrument designed early as 1941 and

used to measure weak signals from a noisy background in applications where signal-to-

noise ratio (SNR) is extremely low [128]. The LIA is able to take a noisy signal and

compare it to a reference signal to selectively extract the weak signal oscillating at the

reference frequency [129]. The instrument is fundamentally composed of two

components: a phase sensitive detector (PSD), and a low pass filter.

The PSD is the critical component in a LIA. The two input signals to the PSD are

the raw signal and the reference signal. The raw signal is the noisy signal where there

exists some weak component signal of interest at a target frequency. The reference

signal is a separate sinusoidal signal whose frequency is equivalent to the target

frequency. Thus, the general form of the raw signal and reference signal can be

represented by the expressions

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𝑋(𝑡)𝑟𝑎𝑤 = 𝑉𝑟𝑎𝑤𝑠𝑖𝑛 (2𝜋𝑓𝑟𝑎𝑤𝑡 + 𝜃𝑟𝑎𝑤) (5)

and

𝑋(𝑡)𝑟𝑒𝑓 = 𝑉𝑟𝑒𝑓 𝑠𝑖𝑛(2𝜋𝑓𝑟𝑒𝑓𝑡 + 𝜃𝑟𝑒𝑓) , (6)

where 𝑉 is amplitude, 𝑓 is frequency and 𝜃 is phase shift for the raw and reference

signals respectively. Equation (5) and equation (6) can also be given in the frequency

domain as

𝑋(𝑓)𝑟𝑎𝑤 =𝛿(𝑓 − 𝑓𝑟𝑎𝑤) − 𝛿(𝑓 + 𝑓𝑟𝑎𝑤)

2

(7)

and

𝑋(𝑓)𝑟𝑒𝑓 =𝛿(𝑓 − 𝑓𝑟𝑒𝑓) − 𝛿(𝑓 + 𝑓𝑟𝑒𝑓)

2 ,

(8)

respectively. Note that frequency domain equations are shown without accounting for

phase shift for simplicity. The PSD passes the raw and reference signals through a

frequency mixer. This is analogous to multiplying the time domain signals or performing

a convolution in the frequency domain. The resulting output of the PSD is

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𝑌(𝑡) =1

2𝑉𝑟𝑎𝑤𝑉𝑟𝑒𝑓[𝑐𝑜𝑠(2𝜋𝑓𝑟𝑎𝑤𝑡 − 2𝜋𝑓𝑟𝑒𝑓𝑡 + 𝜃𝑟𝑎𝑤 − 𝜃𝑟𝑒𝑓)

− 𝑐𝑜𝑠(2𝜋𝑓𝑟𝑎𝑤𝑡 + 2𝜋𝑓𝑟𝑒𝑓𝑡 + 𝜃𝑟𝑎𝑤 + 𝜃𝑟𝑒𝑓)]

(9)

in the time domain or

𝑌(𝑓) =1

4(𝛿(𝑓 − 𝑎) + 𝛿(𝑓 + 𝑎) − 𝛿(𝑓 − 𝑏) − 𝛿(𝑓 + 𝑏)) , (10)

in the frequency domain where 𝑎 = 𝑓𝑟𝑎𝑤 − 𝑓𝑟𝑒𝑓 and 𝑏 = 𝑓𝑟𝑎𝑤 + 𝑓𝑟𝑒𝑓 . Considering the

condition that 𝑓𝑟𝑎𝑤 = 𝑓𝑟𝑒𝑓 , equations (9) and (10) show the output from the PSD has

two frequency components; one at frequency of zero, and another at the sum frequency

of the inputs. This output signal is conditioned by a low pass filter which attenuates

signal components at the sum frequency and its harmonics. Thus, the final output from

the LIA is a DC signal where amplitude is proportional to the reference frequency

amplitude in the raw signal.

4.3 Experimental Setup

A schematic of the experimental setup used in this chapter is shown in Figure 9. A

printed circuit board housing an LED is held by a xyz-stage (i.e., a three axis micro-

adjustable platform structure). The LED is vertically aligned with the sample droplet, an

indium tin oxide (ITO) slide, and a photodiode with an optical filter. To minimize distance

between the LED and photodiode, the LED is positioned as close to the sample droplet

as possible without physical contact.

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Indium tin oxide is commonly used in DMF optical sensing applications due to its

conductivity and transparency [15]. In these experiments, the ITO slide was prepared by

dispensing a 5 cSt silicone oil droplet (Sigma Aldrich, United States) and spreading

gently by gloved finger. The thin silicone oil layer provided the hydrophobic coating that

would be present in DMF devices such as that presented in Chapter 3. The silicone oil

also allowed sample droplets to form a high contact angle and prevent from spreading

onto the ITO slide.

The photodiode used in these experiments was the DET 36A/M (Thorlabs,

United States) silicon based photodiode. This photodiode is sensitive to light

wavelengths in the range of 350 nm – 1100 nm. The photodiode was operated in

photovoltaic mode to minimize dark current. The optical filter is placed between the ITO

slide and photodiode to block the excitation wavelength and pass the longer fluorescent

wavelength. The LED and optical filters are chosen depending on fluorescent

characteristics of the analyte.

The SR830 LIA (Stanford Research Systems, United States) was used for the

presented lock-in based florescence spectroscopy experiments. The LIA took input

current from the photodiode to its internal trans-impedance amplifier configured with a

gain of 106 V/A. Sensitivity of the LIA was set as 50 mV/nA. Time constant was set as

30 milliseconds. Slope of the internal low pass filter was set as 18 dB.

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Figure 9: Schematic of the LIA fluorescence spectroscopy experiment. An LED, sample droplet, optical filter and photodiode are aligned in the vertical plane. The LED is driven by square wave from a function generator. TTL output from the function generator is given as reference signal to the LIA. Output current from the photodiode is the raw input to the LIA.

4.4 Rhodamine Pilot Experiment

A pilot experiment using a fluorescent dye called rhodamine B (Sigma Aldrich)

was performed to validate the experimental setup. The rhodamine B fluorescent dye

emits visible light at a wavelength of 627 nm (i.e., red) when excited at 553 nm (i.e.,

green). The rhodamine dye was mixed in aqueous droplets to test concentrations

ranging 0.5 µM to 67 µM. Droplets were pipetted onto the ITO slide at a fixed volume of

5.0 µL. A green LED was driven by a 2500 Hz square wave from a function generator.

The FEL0600 long-pass filter (Thorlabs, United States) with cut-on wavelength of 600

nm was used to pass only fluorescent light onto the photodiode. Between each trial the

sample droplet was removed and a new droplet was pipetted. The photocurrent

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measured by the LIA versus rhodamine B concentration in aqueous droplets is plotted

in Figure 10.

The plot in Figure 10 shows a positive correlation between fluorescent dye

concentration and photocurrent. The logarithmic trend is characteristic of photodiodes

operated in photovoltaic mode. The response can be made increasingly linear by

reverse-biasing the photodiode and operating in the photoconductive mode although the

drawback is increased dark current. The results of this pilot experiment validated

performance of the experimental setup.

Figure 10: Lock-in amplified photocurrent against rhodamine B concentration in 5.0 µL aqueous droplets. The mean photocurrent and corresponding standard deviation of n = 3 repeated measurements are shown as a function of rhodamine B concentration.

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4.5 Antibiotic Detection

The following experiments measure concentration of ciprofloxacin in milk

droplets. Ciprofloxacin is a widely used antibiotic to treat cattle and is strictly regulated

in dairy products [130]. Ciprofloxacin hydrochloride (Fisher Scientific, United States),

was dissolved in two percent milk bought from a local vendor to produce solutions of

concentrations ranging 0.01 mM to 1.00 mM. Previous studies have demonstrated

fluorescence of ciprofloxacin to emit at 440 nm (i.e., blue) when excited at 280 nm (i.e.,

ultraviolet) [131], [132]. The LED used in this work was the commercially available

VLMU60CL00-280–125 (Vishay Semiconductors, United States) with peak wavelength

of 280 nm and output power of 2.4 mW. The LED was driven by a 2500 Hz square

wave. The Edmund Optics 86–339 band-pass filter (Edmund Optics, United States)

centered at 440nm with bandwidth of 40 nm was placed above the photodiode. The

photocurrent measured by the LIA is plotted against ciprofloxacin concentration in

Figure 11.

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Figure 11: Lock-in amplified photocurrent against ciprofloxacin concentration in 5.0 µL milk droplets. The mean photocurrent and corresponding standard deviation of n = 5 repeated measurements are shown as a function of ciprofloxacin concentration.

The results in Figure 11 show an increasing photocurrent with increasing

ciprofloxacin concentration in 5.0 µL milk droplets. The lowest ciprofloxacin

concentration experimentally measured is 0.01 mM. The slope of the response curve in

Figure 11 corresponds to a measurement sensitivity of 1.39 nA/mM. The limit of

detection can then be calculated as the ratio of three times the standard deviation of the

blank reading to detection sensitivity [37]. This yields a limit of detection of 0.015 mM.

This 0.015 mM limit of detection achieved with LIA measurement is improved from a

similar experiment using continuous microfluidics and electrophoresis separation of

filtered milk to achieve a limit of detection of 0.19 mM [58].

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4.6 Effect of Droplet Volume

The LIA fluorescent detection of ciprofloxacin in milk was performed with varied

droplet volumes to investigate the effect on fluorescent output. These results are shown

in Figure 12. The results showed a general increase in LIA measured photocurrent with

droplet volume which suggested increased fluorescent intensity with droplet volume.

Previous studies have demonstrated that increased fluorescence intensity is not directly

proportional to droplet volume [133]. Instead, the relation between droplet fluorescence

intensity and volume is characterized by a complex interaction between scattering, ray

focusing and absorbance within the droplet [133], [134]. The trend shown in Figure 12 is

very likely to reverse at larger droplet volumes where absorbance of the bulk medium

becomes more dominant and the effect of ray focusing is minimized [134].

The increasing fluorescent intensity of ciprofloxacin with milk droplet volumes on

the microlitre scale is well-suited to open configuration DMF devices such as that

demonstrated in Chapter 3. By comparison to closed configuration DMF, the open

configuration is preferred to handle larger droplet volumes [135]. Thus, the use of an

open configuration DMF device for dairy testing shows advantages in overcoming

biofouling and optimizing fluorescence detection.

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Figure 12: Lock-in amplified photocurrent against ciprofloxacin concentration in milk droplets of volumes: (a) 7 µL, (b) 9 µL, (c) 11 µL and (d) 13 µL. The mean photocurrents and corresponding standard deviations of n = 3 repeated measurements are shown as a function of ciprofloxacin concentration.

4.7 Chapter Conclusion

In this chapter we demonstrated an LIA fluorescence spectroscopy method for

measuring concentration of ciprofloxacin in milk droplets. This detection method is label-

free and does not require any separation of the antibiotic from the bulk milk droplet.

Using UV-Vis fluorescence spectroscopy, a limit of detection of 0.015 mM for

ciprofloxacin in milk droplets was achieved. At the molar mass of 331.35 g/mol and milk

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density of 1.03 kg/L [136], this limit of detection translates to 5 ppm which is comparable

to the required regulatory limit of detection of 0.1 ppm [130]. This UV-Vis spectroscopy

detection can be extended to multiple antibiotics regulated in dairy milk [37], [38], [40],

[61].

The presented method demonstrates label-free optical detection which is well-

suited to integration on DMF devices. The trend between droplet volume and

fluorescent intensity also lends itself to potential optimization on a DMF device. Thus,

the results of this work are important to demonstrating a viable method for antibiotic

detection in milk droplets which is necessary for future development of a DMF dairy

testing device.

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5 Conclusions

This final chapter provides a review of the contributions of this thesis. Each chapter

is briefly summarized. The impact of this experimental work is stated along with

recommendations for future work.

5.1 Summary of Contributions

This thesis demonstrated the fundamental functionalities required by a digital

microfluidic device for on-site dairy testing. The functionalities of automated milk droplet

actuation and antibiotic detection in milk droplets were developed and studied.

The first chapter of this thesis detailed the problem faced by dairy farmers due to

the current practice of antibiotic residue testing. The value of an on-site dairy tester to

use during milk collection was shown to protect the farmer and dairy industry from loss

of money and milk. Current commercially available methods were shown to be unviable

for use during milk collection due to manual processes and long response times. Digital

microfluidic technology was shown to be an appealing solution due to strengths in

automation, parallelization and reconfigurability. The application of digital microfluidics

to dairy testing was met with two immediate challenges in overcoming biofouling to

actuate milk droplets and antibiotic detection in milk droplets. The work scope of this

thesis was to overcome these two immediate challenges and thereby enable the

adaption of digital microfluidics to dairy testing.

The second chapter provided a detailed literature review of the existing technology

used in dairy testing and also about DMF. The importance of antibiotic regulation in

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dairy milk was discussed. The current testing methods used in laboratories and their

limitations for adaption in on-site solutions were stated. Next, commercially available on-

site dairy sensors and their underlying technologies were detailed. Specifically, the

advancement of traditional microfluidic MCE devices was discussed. These on-site

dairy sensors were shown to be unsuitable for dairy testing during milk collection due to

need for manual procedures, long response times and lack of robustness. DMF

technology and its advantages were introduced. The theoretical actuation of droplets

and complications presented by biofouling were described. DMF compatible detection

methods and the particular appeal of fluorescence spectroscopy for this work were

shown.

The third chapter addressed issues of biofouling and integration faced in

developing a DMF device for dairy testing applications. A fully integrated DMF device

was designed to leverage advantages in automation, parallelization and

reconfigurability. A modular PCB hardware, event driven firmware and versatile control

software was demonstrated in a single integrated DMF device. Experimental studies

measuring droplet velocities were conducted to determine an optimized architecture for

actuation of milk droplets in an air filler medium. The use of a closed DMF configuration

was found unsuitable for bio-fluid actuation due to contact between the sample and

hydrophobic layer of the top plane of the device. Thus, the open configuration was

proven to be the desired configuration. Experiments comparing performance of a gel-

based PDMS dielectric and stretched parafilm dielectric showed the surface roughness

of PDMS was especially disadvantageous in open configurations. The developed DMF

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device showed automated continuous milk droplet actuation when using an open

configuration, parafilm dielectric and silicone oil coating.

The fourth chapter addressed the issue of antibiotic detection in milk droplets. This

issue was the second required functionality of a digital microfluidic device for dairy

testing. Digital microfluidic technology was shown to be disadvantaged compared to

traditional microfluidics in the domain of sample separation. Digital microfluidic detection

applications were shown to often rely on label molecules which are undesirable due to

cost and complexity. To address this, a lock-in amplifier instrument was used to

enhance the fluorescence spectroscopy detection method which is widely compatible

with digital microfluidic devices. Using lock-in amplified UV-Vis fluorescence

spectroscopy, the ciprofloxacin antibiotic was detected label-free in milk droplets without

any chemical separation. Experiments investigating fluorescent intensity by droplet

volume showed a trend favourable for open configuration digital microfluidics. Hence, a

method for antibiotic detection in milk droplets compatible with digital microfluidics was

demonstrated.

In summary, the work of this thesis has successfully demonstrated the most

fundamental functionalities, with respect to actuation and detection, for adaption of

digital microfluidics to dairy testing applications. Thus, this thesis provides the

foundation for designing a digital microfluidic dairy device for antibiotic detection.

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5.2 Future Works

The linearity and sensitivity of the fluorescent intensity versus antibiotic

concentration response shown in Chapter 4 has potential for improvement by operating

the photodiode in photoconductive mode. By reverse-biasing the photodiode, the width

of the semiconductor depletion region is increased. Consequently, the response has

greater sensitivity and linearity. Operation in photoconductive mode often has the

drawback of greater dark current and therefore a greater noise floor. However, the dark

current effect may be negated by the lock-in amplified measurement.

Having had this thesis demonstrate milk droplet actuation and milk droplet antibiotic

detection on separated systems, an intriguing future work will be the combination of

these functionalities in a single device. A custom fixture should be developed to

minimize the distance between an LED, milk droplet and photodiode. Use of multiple

LEDs and photodiodes has potential for detecting multiple regulated antibiotics in milk

as has been done in some traditional microfluidic devices [38]–[40], [61]. This proposed

future work will be very impactful in realizing a complete digital microfluidic on-site dairy

tester.

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