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Original Research ARTICLE

Front. Microbiol., 14 October 2014 | https://doi.org/10.3389/fmicb.2014.00537

Laser-induced speckle scatter patterns in Bacillus colonies

Huisung Kim1, Atul K. Singh2, Arun K. Bhunia2 and Euiwon Bae1*
  • 1Applied Optics Laboratory, School of Mechanical Engineering, Purdue University, West Lafayette, IN, USA
  • 2Molecular Food Microbiology Laboratory, Department of Food Science, Purdue University, West Lafayette, IN, USA

Label-free bacterial colony phenotyping technology called BARDOT (Bacterial Rapid Detection using Optical scattering Technology) provided successful classification of several different bacteria at the genus, species, and serovar level. Recent experiments with colonies of Bacillus species provided strikingly different characteristics of elastic light scatter (ELS) patterns, which were comprised of random speckles compared to other bacteria, which are dominated by concentric rings and spokes. Since this laser-based optical sensor interrogates the whole volume of the colony, 3-D information of micro- and macro-structures are all encoded in the far-field scatter patterns. Here, we present a theoretical model explaining the underlying mechanism of the speckle formation by the colonies from Bacillus species. Except for Bacillus polymyxa, all Bacillus spp. produced random bright spots on the imaging plane, which presumably dependent on the cellular and molecular organization and content within the colony. Our scatter model-based analysis revealed that colony spread resulting in variable surface roughness can modify the wavefront of the scatter field. As the center diameter of the Bacillus spp. colony grew from 500 to 900 μm, average speckles area decreased two-fold and the number of small speckles increased seven-fold. In conclusion, as Bacillus colony grows, the average speckle size in the scatter pattern decreases and the number of smaller speckle increases due to the swarming growth characteristics of bacteria within the colony.

Introduction

Bacterial colonies consist of millions of individual cells interacting with each other in complex ways (Shapiro, 1992; Wimpenny, 1992; Shimada et al., 1995; Ben-Jacob et al., 1998). It is important to understand the mechanism of colony formation and the resulting morphology as it is a key to understand organizations and interactions among bacterial cells within a colony. The colony morphology is highly influenced by the shape of individual cells, cell wall components (peptidoglycan, teichoic acid, lipopolysaccharide), the extracellular components and appendages (flagella, fimbriae, curli), and cellular response to the environmental cues including nutrient availability, oxygen and other gases, salt, acidity, alkalinity, temperature, etc. (Nagai et al., 1971; Granek and Magwene, 2010). Therefore, the colony morphology of different bacteria could be used as a foundation for differential characterization using an interrogating tool.

Historically, bacterial colony pattern formation has drawn significant interest among diverse research fields. Microbiologists were more interested in determining how bacterial response to the environmental factors such as nutrient and agar hardness affect colony formation, while the physicist were aiming to recreate the colony formation scenario by using theoretical models. Shapiro and Wimpenny first observed bacterial colony formation in time and space (Shapiro, 1992; Wimpenny, 1992) and since then, many other researchers employed both experimental (Shimada et al., 1995; Ben-Jacob et al., 1998; Bees et al., 2000; Stecchini et al., 2001; Kaito and Sekimizu, 2007; Pipe and Grimson, 2008) and theoretical models (Kawasaki et al., 1997; Cohen et al., 1999; Kozlovsky et al., 1999; Lega and Passot, 2003) to explain such phenomenon. Among the various organisms tested, a majority of the study used Bacillus spp. as a model due to their swarming growth characteristics. Swarming colonies can generate diverse spatio-temporal patterns due to their reproduction and spreading mechanisms (Harshey, 2003). Therefore, we also studied Bacillus as a model organism to correlate the swarming colony morphology to the optical light scattering and speckle effect.

Since the first reports (Bae et al., 2007; Banada et al., 2007), optical light scattering of colony have expanded to differentiate diverse bacterial genera. The remarkable resolving power of the BARDOT originates from the accumulation and amplification of both microscopic structural and biochemical differences that exist among different bacterial colonies through an interrogating laser beam. When the laser beam passes through the bacterial colony, both 3D morphological and optical characteristics are integrated into 2D outgoing wave and encoding it on the coherent optical wavefront. The wavefront then propagates through near- and far-fields governed by the diffraction integral to form distinctive forward scattering pattern which serves as an optical “fingerprint.”

Elastic light scatter (ELS) has been used by our group for bacterial colony differentiation and identification (Bae et al., 2007, 2011; Banada et al., 2009; Huff et al., 2012; Singh et al., 2014). Recently we have used this technology for differentiating Bacillus cereus (an important food poisoning species) and compared its colony scattering pattern with another ubiquitous species, Escherichia coli (Singh et al., submitted). Bacillus is highly motile and considered a swarming bacterium, which shows greater mobility on solid agar. Among the Bacillus spp., surprisingly, only B. polymyxa expressed typical ELS patterns of concentric rings and spokes consistent with other bacterial genera: Listeria, Salmonella, Vibrio, Escherichia, and Staphylococcus (Bae et al., 2007; Banada et al., 2009; Huff et al., 2012; Singh et al., 2014). While all other Bacillus species tested showed random speckles overlaid with some circular ring patterns (Singh et al., submitted). The scattering patterns of B. subtilis and B. polymyxa have shown significant differentiating characteristics. In this paper, we investigated the different optical properties of these two Bacillus species; (i) to understand how B. subtilis and B. polymyxa construct their colony using recently developed Integrated Colony Morphology Analyzer (ICMA) (Kim et al., 2013); (ii) to compare the theoretical prediction of ELS patterns with experimental data; and (iii) to calculate the speckle statistics to quantitatively correlate the optical phase modulation into the structure of the bacterial colony.

Materials and Methods

Sample Preparation

Bacillus subtilis ATCC 6633 (B. subtilis), Bacillus polymyxa B719W (B. polymyxa), Bacillus cereus ATCC 14579 (B. cereus), and Bacillus thuringiensis DUP6044 (B. thuringiensis) cultures were used in this study. Cultures were inoculated in brain heart infusion (BHI) broth (Difco, MD, USA) and incubated at 37°C for overnight (16 h) with 130 rpm shaker, 10-fold serially diluted in 0.2 mM phosphate buffered saline, pH 7.0 (PBS) and diluents were plated on BHI and phenol red mannitol (PRM) agar plates (Becton Dickinson, NJ, USA) to obtain 50–100 colonies. Optical scatter patterns of the colonies were captured using the BARDOT instrument at 6–8 h that corresponds to colony diameter of about 550, 750, and 900 μm, respectively.

Forward Scatterometer

Scatterometer (Figure 1A), consists of laser diode (LD) with 635 nm wavelength that was installed as a light source, and the light source directly illuminates a single bacterial colony grown on semi-solid agar plate. The diffracted light is captured using detector (CMOS camera, PL-B741, ON, Canada) with 1280(H) × 1024(V) pixels, 6.7 × 6.7 μm pixel pitch which is located after the semi-solid agar plate with distance z. Motorized 2 axis lateral stage was integrated to the system, and the semi-solid agar plate was put on the 2 axis lateral stage for a full automatic measurement of optical scatter pattern. The Bacillus colonies were then picked from the plate, grown briefly (4 h) in BHI broth at 37°C and analyzed by multiplex PCR (mPCR) assay.

FIGURE 1
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Figure 1. Schematic diagram of the experimental setup. (A) Schematic diagram of BARDOT instrument, laser diode (LD) with 635 nm wavelength is used as a light source and directly impinging the single bacterial colony grown on an agar plate. Spatially scattered light is captured by a 2-D detector. (B) Schematic diagram of ICMA, in-situ morphology and optical density map of bacterial colony measurement unit.

DNA Extraction and mPCR

Total DNA was extracted by boiling cultures as described earlier (Ngamwongsatit et al., 2008). mPCR was performed using gyrB gene-specific primers (BcF: 5′ GTTTCTGGTGGT TTACATGG3′; BcR: 5′TTTTGAGCGATTTAAATGC 3′) and cry gene-specific primers (K5F: 5′AGG ACCAGGATTTACAGGAGG 3′; K3R: 5′ GCTGTGACACGAAGGATATAGCCAC 3′) (Kuo and Chak, 1996; Manzano et al., 2003). The mPCR reaction mixture contained 200 μM of each dNTP, 2.5 mM of MgCl2, 0.8X GoTaq Flexi buffer, 1U of GoTaq Flexi DNA polymerase (Promega), 0.2–0.3 μM of primers, 60–90 ng of template DNA and the reaction condition was optimized (Henegariu et al., 1997; Lorenz, 2012). Ultra-pure sterile water was used as negative control. PCR reaction was only considered valid when control reaction was either positive or negative as appropriate and 16S rRNA gene was positively amplified with all DNA templates. All amplicons were analyzed on 1.2% agarose gel.

Integrated Colony Morphology Analyzer (ICMA)

As shown in Figure 1B, the laser confocal displacement meter (CDM) (Keyence, LT9010M) is located at the top and attached to a linear horizontal translation stage (Edmund Optics, NJ, USA) in order to position the probing laser beam (λ = 670 nm) along the vertical z axis and to focus it on the surface of colony. A motorized 2D lateral stage translated the Petri dish in the x-y plane to align the diagnostic laser beam with each selected bacterial colony to obtain their 3-D profiles. Two linear motors (850G-HS) connected to the ESP 300 multi-axis closed-loop controller (Newport, NY, USA) with the specification of a 42 mm maximum stroke and a 0.1 mm minimum step size control the movement of the x-y stage. This instrument implements a high accuracy surface scanning method by using a laser light source with a Gaussian beam spot of approximately 2 μm. The position of the doublet lenses is controlled by a tuning fork moving up and down at high frequency. When the beam was focused on the sample (colony) surface, the reflected light traveled back along the original optical path and was directed toward the pinhole to produce the highest level of intensity on the light receiving element. If the laser is unfocused, some of the reflected light would be occluded at the pinhole. Therefore, the relative height of the measured surface was registered by the sensor positioned at the bottom of the tuning fork, and the values are calculated and converted to an absolute height value (Keyence-Corporation, 2006).

A micro-objective lens (Bausch & Lomb, 20x, N.A. 0.4) is placed just below the Petri dish to focus the transmitted light onto the active area of the photodiode (Hamamatsu, S1087) (Figure 1B). This photodiode offered a low background noise (10 pA) with a wide dynamic range and provided a spectral response from 320 to 730 nm with the peak sensitivity at 560 nm. The active area for this photodiode is 1.3 × 1.3 mm2, providing a photo sensitivity of 0.19 A/W for the incoming laser from the CDM sensor head on which a custom built active components driven I-V converter and preamp were installed at a preamp section. A custom built micro controller unit (MCU) (AVR128, Atmel) was used as a data acquisition unit. Through use of the MCU's internal 10 bit A/D conversion, all signals from the photodiode circuit and CDM were captured and transferred simultaneously to the PC by means of serial communication. All sequences were controlled by a custom built graphic user interface (GUI) at the PC, which was developed using Microsoft Visual Studio 2008 and both were analyzed and visualized in MATLAB.

Modeling Speckle Effect From Elastic Light Scattering

The bacterial colony and a semi-solid media are positioned at the aperture plane, and the forward scattering pattern is captured at the image plane, defined as (xa, ya) and (xi, yi), respectively. A bacterial colony is modeled as a bell curve shape with tailing edge (Gaussian-like profile) where colony center height and radius is defined as H0 and rc, respectively. Based on Rayleigh and Sommerfeld formation of diffraction, and Fresnel diffraction approximation (Bae et al., 2007, 2010), intensity of electric field at aperture and image plane is derived as Equations (1) and (2), respectively, where distance between aperture plane to a point at image plane, rai is assumed as Equation (3).

Ea(xa,ya,z)=E0exp[(xa2+ya2)ω2(z)]exp(ikz)                           exp[ik(xa2+ya2)2R(z)]    (1)
      Ei(xi,yi)=1iλt(xa,ya)Ea(xa,ya)exp[ikΦ(xa,ya)]                         exp[ikrai]raicosθdxadya    (2)
               rai=[zi2+(xaxi)2+(yayi)2]12                     zi[1+12(xaxizi)2+12(yayizi)2]    (3)

Since previous researchers focused on structural morphology of bacterial colony such as elevation and colony diameter, the colony was modeled as smooth curve with Gaussian profile function without considering surface roughness. In reality, a cross section of bacterial colony showed the accumulation of densely packed multiple layers of bacterial cells (Banada et al., 2009; Bae et al., 2010; Suchwalko et al., 2013; Marcoux et al., 2014). Furthermore, Bacillus colonies also showed some degree of surface roughness (Figures 2, 3). To simplify the modeling, surface roughness is generated by random signal with colony area, and superposed to the colony morphology. Considering the surface roughness of the colony, intensity of electric field at image plane is simplified as Equation (4).

Ei(xi,yi)=CT(xa,ya)exp[iΦr]exp[iΦc]exp[i(Φg+Φs)]exp[2πi(fxxa+fyya)]dxadya    (4)

where T is amplitude modulator; fx and fy is defined as xi/(λz2) and yi/(λz2), known as a spatial Fourier frequency; Φr, Φq, Φg, and Φs is radial, quadratic, Gaussian, and surface roughness phase component respectively, and defined as:

Φr(xa,ya)=k(xa2+ya2)2R    (5)
Φq(xa,ya)=k(xa2+ya2)2zi    (6)
Φg(xa,ya)=k(nbac1)H0exp[(xa2+ya2)rc2]    (7)
Φs(xa,ya)=k(random(xa,ya))where(xa2+ya2<rc2)    (8)
FIGURE 2
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Figure 2. Phase contrast images of the B. subtilis on (A) BHI and (B) PRM where colony shows swarming growth characteristics. For comparison, B. polymyxa on (C) BHI and (D) PRM are shown where colony forms a circular shape.

FIGURE 3
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Figure 3. Profile and OD map acquired from ICMA. Top row displays the profile map of (A) B. subtilis ATCC 6633 colony and (B) B. polymyxa B719W colony, and (C) profile cross section of both species. Bottom row shows the OD map of (D) B. subtilis ATCC 6633 colony and (E) B. polymyxa B719W colony, and (F) OD cross section of both species on PRM.

The summation of four phase components,Φoverall is working as phase modulator for the propagating light. The amplitude modulator T is derived as:

T(xa,ya)=exp[(xa2+ya2)ω2(z)]EoutE0=exp[(xa2+ya2)ω2(z)](1rairbac)(1rk)2l(1rbacagar)    (9)
Φoverall=Φr+Φq+(Φg+Φs)    (10)

Coefficient of Equation (4), C is derived as:

C=E0exp(iknagarΔagar)exp(ikH0)exp[ik(z+zi)]exp[ik(xi2+yi2)/2zi]iλzi    (11)

where Δagar and nagar is defined as thickness of agar and refractive index of agar respectively.

Speckle Analysis

To provide quantitative speckle analysis, a MATLAB code was constructed utilizing an image processing toolbox V2.6 (Vliet, 2014). A radial Gaussian blur was applied to the raw image to apply a low pass filter that eliminates the objects while keeps the slow change in the background, and the blurred image was subtracted from the raw image to remove the background noise. The subtracted image was binarized with locally adaptive threshold using approximation of gradient of background intensity to eliminate the external lighting and local CMOS sensor sensitivity characteristics effect on the image. Then, each speckle was segmented, grouped, and labeled. Number of pixels (size of the speckle) and feret diameter (Merkus, 2009) of each segmented group was computed, and analyzed.

Results

Here, we report how colony morphology correlates with its speckle patterns using both theoretical and experimental approaches. Thus, each colony was first interrogated by ICMA and phase contrast microscopy to record height, transmittance and morphology.

Colony Development Profiles

The phase contrast microscopic (PCM) images of colonies of B. subtilis and B. polymyxa on both BHI and PRM were contrasting (Figure 2). B. subtilis colony has an irregular boundary with bumpy and uneven surface structure on both media (Figures 2A,B). Due to the limitation of phase contrast microscopic setup, the 3-D elevation cannot be interpreted with current image but B. subtilis shows a representative swarming colony characteristics, where spatially localized variations of bacterial cell densities are observed. Meanwhile, B. polymyxa had symmetrical circular boundary with relatively smooth surface curvature (Figures 2C,D). As the PCM result showed, the colony forming characteristics of B. polymyxa was drastically different from the majority of other Bacillus species including B. subtilis, B. cereus, and B. thuringiensis.

Comparison of Transmittance and Elevation Profile

To compensate the phase contrast microscope image, ICAM was utilized to acquire spatially resolved optical characteristics from a single colony. Figures 3A,B show the morphology map of B. subtilis and B. polymyxa colony on PRM, respectively from morphology channel of ICMA; whereas panel (d) and (e) show their corresponding spatially resolved transmittance in optical density (OD) units with 670 nm light source. Colonies of both species on PRM agar were captured after 7 h of growth, when the center diameter of B. polymyxa colony reached to approximately 800 μm. Similar to the PCM result, morphology map by ICMA revealed that boundary of B. subtilis colony was irregular, while, B. polymyxa colony had near circular symmetrical boundary (Figures 3A,B). Comparison of morphology cross section for the both species at their center area showed that B. subtilis colony had random bumpy profile with rough surface, while B. polymyxa colony had bell curve-like profile with relatively smooth surface (Figure 3C). B. subtilis colony had approximate 890 μm cross sectional diameter and 57 μm of center peak height, while, B. polymyxa colony had 814 μm diameter and 66 μm of colony center height. Considering the colony aspect ratio (colony center height to diameter ratio) of each species, B. subtilis (1:15.6) colony had more flat cross sectional profile than B. polymyxa (1:12.4) at the same diameter. Furthermore, the 2-D transmittance map (cross-sectional OD profile) of both species shows more distinctive characteristics, which can be attributed to colony morphology and opacity (Figures 3C,F). Since the OD of BHI agar plate alone at 670 nm was approximately 0.2, cross section of the OD result had 0.2 offset. Cross section of B. subtilis colony OD fluctuates from 0.24 to 0.41, while B. polymyxa colony had OD with maxima 0.29. Assuming that each species of bacterial cell had identical optical characteristic, this irregularity and randomness of OD can be ascribed to different spatial cell density that is translated into variation in light absorption. In addition, surface roughness of the B. subtilis colony can be modeled as variation in reflected and transmitted light intensity (Figure 3).

ELS Measurement

In previous studies, optical forward scattering pattern or ELS of Salmonella, E. coli, and Staphylococcus showed characteristics symmetric or concentric circle with some radial spokes (Banada et al., 2009). However, forward scattering pattern of Bacillus species (except B. polymyxa) showed speckle pattern (Figures 4A, 5). Diffraction pattern of B. subtilis colony is consisted of only small sized random speckle, while, B. polymyxa shows concentric circular pattern (Figure 4). To verify the time resolved speckle development of Bacillus species on their forward scattering pattern, B. subtilis, B. cereus, and B. thuringiensis were selected and their diffraction patterns were measured after 6–8 h of growth using BARDOT (Figure 5). As the incubation time increased from 6 to 8 h, the diffraction patterns also evolved to fully developed speckles, i.e., structured patterns progressively became unstructured random speckles. All three Bacillus species displayed similar trend as the incubation time increased where average speckle numbers decreased.

FIGURE 4
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Figure 4. Elastic light scatter (ELS) patterns on PRM agar for (A) B. subtilis ATCC 6633, and (B) B. polymyxa B719W; (C) Multiplex PCR (mPCR) for differentiation of Bacillus cereus-group strains (Lane 1–5) from other Bacillus species (Lane 6–11). mPCR resulted a 374 bp PCR product for all Bacillus cereus-group strains and a 1.6 kb size PCR product only for B. thuringiensis. Lane 12 and 13 represents single gene specific amplification for gyraseB gene in Bacillus cereus and cry gene in Bacillus thuringiensis. mPCR was performed with gyrase B gene-specific and cry protein gene-specific primers.

FIGURE 5
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Figure 5. Time-resolve ELS patterns for three different Bacillus species: B. subtilis, B. cereus, and B. thuringiensis on PRM agar. As the incubation time increases from 6 to 8 h, ELS pattern evolves to a fully developed speckle when an average speckle diameter decreases.

Comparative Analysis of Experiment with Simulation

To investigate the effect of surface roughness on forward scattering pattern, other components of models are kept constant for Equations (5)–(11). The effect of random surface phase component (Φs) on forward scattering pattern was determined (Figure 6). Figure 6A shows the forward scattering pattern prediction when the surface phase component was equal to zero which means, the colony surface was devoid of any random structures. The predicted scatter image contained concentric ring patterns with small bright ring at the center and the thickness of rings increased as they moved outwardly. To mimic the random surface roughness effect, Equation (8) was adopted which is a random function multiplied by the wave number k, and is only influenced by bacterial colony region. The maximum amplitude of the random function for Equation (8) was chosen as 1/150, 1/100, and 1/80 of colony center height for fine, medium, and coarse surface roughness, respectively. The surface roughness component (Φs) is added to Gaussian phase component (Φg), and worked as a part of phase modulator, which can deform the incident wave front. Predicted forward scatter patterns are shown for fine (Figure 6B), medium (Figure 6C), and coarse surface roughness (Figure 6D). For a diffraction pattern prediction with fine surface roughness effect, relatively larger size speckles and less number of speckles were generated, and still had concentric circle pattern. As the surface roughness increased, the size of the speckle decreased and higher number of speckles were generated, and formed a random speckle pattern rather than concentric circle pattern as predicted.

FIGURE 6
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Figure 6. Theoretical analysis of speckle development based on the random phase shift (φs) of scalar diffraction theory. Phase shift was modified as (A) 1/200, (B) 1/150, (C) 1/100, and (D) 1/80 and their simulated scatter patterns show similar trend with the experiment.

Figure 7 shows the comparison of theoretical speckle development on diffraction pattern by surface roughness and that from experiment. The results were plotted for speckle area vs. the number of speckles. For the prediction, the maximum amplitude of the random function for Φs were set as 1/200, 1/150, and 1/100 of B. cereus colony center height for fine, medium, and coarse roughness, respectively. As the theoretical model moved from coarse () to fine () surface roughness, the model predicts decreasing average speckle size with increasing numbers. Similar trend was observed in experiment with B. cereus ATCC14579 incubated from 6 h () to 8 h (Δ) (Figure 7A). For B. thuringiensis DUP6044, Φs was changed to 1/180, 1/130, and 1/100 of colony center height and an excellent agreement between theory and experiment was evident (Figure 7B). For example, coarse surface roughness () and 9 h incubation (Δ) showed almost similar trend in average speckle size and the numbers.

FIGURE 7
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Figure 7. Comparison of theoretical speckle development on diffraction pattern by surface roughness and that of experimental time resolved result for B. cereus and B. thuringiensis. For prediction, the maximum amplitude of random function of surface roughness was adopted as (A) 1/200, 1/150, and 1/100 (B) 1/180, 1/130, and 1/100 of colony center height for fine, medium, and coarse surface roughness, respectively.

Discussion

Understanding bacterial growth on a solid surface is important for biophysicist, microbial ecologist, and food microbiologist for better insight of colony development and its ecological and virulence properties. In context to virulence attributes of colony, small colony variants (SCVs) of different bacteria are often considered more virulent facilitating persistence and recurrent infections (Proctor et al., 2006). Harshey (2003) wrote an excellent review on how bacteria form colony in four different ways (swarming, gliding, twitching, and sliding). Our motivation to this study was to correlate the unique growth characteristics of Bacillus species to the optical speckle theory and help understand colony growth dynamics. Bacillus has long been used as a model to study the environment dependent variations in growth patterns (Shimada et al., 1995; Ben-Jacob et al., 1998; Bees et al., 2000; Stecchini et al., 2001; Kaito and Sekimizu, 2007; Pipe and Grimson, 2008). However, recent application of optical scattering-based bacterial colony interrogation requires different perspective for fundamental understanding of scatter pattern generation and colony morphology.

Previous studies have shown that availability of nutrients and agar concentration affect the distribution/propagation of cells within a colony (Bae et al., 2011). However, the published studies on colony scatter pattern did not report theoretical interpretation of speckle pattern formation by a colony. To the best of our knowledge, this is the first report of theoretical interpretation of speckle pattern formation by Bacillus colony, which is largely attributed to the roughness of bacterial colony. The surface roughness is believed to be arisen from the swarming behavior of the Bacillus cells during colony formation. ICMA and PCM measurements revealed that B. subtilis generates more rough surface morphology than the B. polymyxa (Figures 2, 3).

For theoretical comparison, ICMA measurement was critical since the scalar diffraction theory required accurate description of the amplitude and phase modulation component of Equations (1)–(11). Both qualitative trend and quantitative measurement showed good agreement (Figure 7). Both theoretical model and the experimental evidence indicate that as bacteria grow, the speckle size decreases and the number increases. Furthermore, the quantitative comparison also revealed that as surface roughness changed from fine to coarse, the number of speckle increased 7 (B. cereus) to 10 (B. thuringiensis) -fold. Similar quantitative trend was observed for two other bacterial species: B. cereus and B. thuringiensis. In future, this information could be used to provide fundamental understanding of inverse scattering method for analyzing bacterial colony formation since size and the number of speckle correlate with incubation time and surface roughness.

The light scattering sensor discussed in this study was successfully used for detection of bacterial pathogens including Listeria monocytogenes (Banada et al., 2007, 2009), Vibrio spp. (Huff et al., 2012), Salmonella serovars (Singh et al., 2014), E. coli O157:H7 (Tang et al., 2014), and Bacillus spp. (Singh et al., submitted). However, these studies did not investigate if mathematical modeling could be used to explain resulting scatter patterns of colonies. Here we focused on developing and comparing the computational model for B. subtitis ATCC 6633 and B. polymyxa B719W for speckle formation and its resultant effect on the experimental scatter pattern. Such in silco study would be of great significance for extrapolating the colonial properties of highly virulent Bacillus species such as Bacillus anthracis, a causative agent of anthrax that requires a high containment facility for handling.

Rather than utilizing specific labeling reagents, proposed method adopted the combination of a laser light and a 2D CMOS sensor to transform the both 3-D macroscopic and microscopic structures (morphology) and material characteristics (refractive indices) effect into a single 2-D scatter image which can be further analyzed by chemometric methods. The proposed method does not disrupt the colony structure while capturing the scatter pattern, thus can be further used in biochemical, molecular, immunological and mass-spectroscopic methods for confirmation of the cultures.

As the modeling of forward scattering pattern for the bacteria colony shows, the morphology and optical characteristics play major roles into formation of diffraction patterns. Previous studies have shown that availability of nutrients and agar concentration (Bae et al., 2011), and storage condition of the agar plate (Mialon et al., 2012) possibly affect the distribution/propagation of cells within a colony and the resulting diffraction pattern. Furthermore, previous studies (Bae et al., 2007, 2010; Kim et al., 2013) indicate that the forward scattering patterns produced by BARDOT are circular symmetric or concentric circle with some radial spokes for most of the microorganisms (E. coli, Listeria, Salmonella, and Staphylococcus) studied.

The outcome of this study would be helpful in analyzing the growth characteristic and understanding of the colonial behavior on solid agar surface using visual, physical, mathematical and empirical models. The results will also help in development of better scatter signatures based classification algorithm for microbial detection, especially the pathogens and spoilage microbes relevant to food safety, food quality and food security.

Conclusion

Here we report a theoretical modeling and experimental verification of the swarming growth characteristics of Bacillus species using optical scattering technology. To quantify the growth characteristics, PCM and ICMA along with BARDOT were utilized. Scalar diffraction theory coupled with new random phase component provided good agreement with experimental speckle pattern formation. The results indicate that as bacteria grow, their average speckle size decrease and the number of smaller speckle increases due to the swarming growth characteristics of bacteria within the colony.

Conflict of Interest Statement

Euiwon Bae and Arun K. Bhunia are inventors of “System and method for rapid detection and characterization of bacterial colonies using forward light scattering” (US Patent No. 7465560), designated BARDOT, described in this review. The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Acknowledgment

This research was supported through a cooperative agreement with the Agricultural Research Service of the US Department of Agriculture project number 1935-42000-035 and the Center for Food Safety Engineering at Purdue University.

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Keywords: bacterial colony, diffraction, speckle, phase modulation, Bacillus

Citation: Kim H, Singh AK, Bhunia AK and Bae E (2014) Laser-induced speckle scatter patterns in Bacillus colonies. Front. Microbiol. 5:537. doi: 10.3389/fmicb.2014.00537

Received: 02 August 2014; Paper pending published: 01 September 2014;
Accepted: 26 September 2014; Published online: 14 October 2014.

Edited by:

Sophie Jeanson, Institut National de la Recherche Agronomique - INRA, France

Reviewed by:

Folarin Anthony Oguntoyinbo, University of Lagos, Nigeria
Stella Maris Reginensi Rivera, Universidad de la República Oriental del Uruguay, Uruguay

Copyright © 2014 Kim, Singh, Bhunia and Bae. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Euiwon Bae, School of Mechanical Engineering, Purdue University, 585 Purdue Mall, West Lafayette, IN 47907, USA e-mail: ebae@purdue.edu