 Research
 Open Access
 Published:
Development of a mathematical model to estimate intratumor oxygen concentrations through multiparametric imaging
BioMedical Engineering OnLine volume 15, Article number: 114 (2016)
Abstract
Background
Tumor hypoxia is involved in every stage of solid tumor development: formation, progression, metastasis, and apoptosis. Two types of hypoxia exist in tumors—chronic hypoxia and acute hypoxia. Recent studies indicate that the regional hypoxia kinetics is closely linked to metastasis and therapeutic responses, but regional hypoxia kinetics is hard to measure. We propose a novel approach to determine the local pO_{2} by fusing the parameters obtained from in vivo functional imaging through the use of a modified multivariate Krogh model.
Methods
To test our idea and its potential to translate into an in vivo setting through the use of existing imaging techniques, simulation studies were performed comparing the local partial oxygen pressure (pO_{2}) from the proposed multivariate image fusion model to the referenced pO_{2} derived by Green’s function, which considers the contribution from every vessel segment of an entire threedimensional tumor vasculature to profile tumor oxygen with high spatial resolution.
Results
pO_{2} derived from our fusion approach were close to the referenced pO_{2} with regression slope near 1.0 and an r^{2} higher than 0.8 if the voxel size (or the spatial resolution set by functional imaging modality) was less than 200 μm. The simulation also showed that the metabolic rate, blood perfusion, and hemoglobin concentration were dominant factors in tissue oxygenation. The impact of the measurement error of functional imaging to the pO_{2} precision and accuracy was simulated. A Gaussian error function with FWHM equal to 20 % of blood perfusion or fractional vascular volume measurement contributed to average 7 % statistical error in pO_{2}.
Conclusion
The simulation results indicate that the fusion of multiple parametric maps through the biophysically derived mathematical models can monitor the intratumor spatial variations of hypoxia in tumors with existing imaging methods, and the potential to further investigate different forms of hypoxia, such as chronic and acute hypoxia, in response to cancer therapies.
Background
The oxygen concentration in normal tissue is maintained in a steady state, where the oxygen diffused from the capillaries meets the metabolic demand of the surrounding cells. Disrupting this balance, such as in wound repair for extra oxygen demand, triggers physiological angiogenesis. The nascent vessel sprouting and pruning from the existing vessel network in physiological angiogenesis are tightly regulated. If the disruption is severe enough, necrosis or apoptosis develops, resulting in a stroke or myocardial infarction. Unlike physiological angiogenesis, tumorinduced angiogenesis is uncontrolled, resulting in a tortuous, leaky, and dilated microvasculature. This dysfunctional microvasculature cannot supply the oxygen demand from tumor cells, and leads to a spatiotemporal heterogeneous hypoxia distribution in tumor [1]. The hypoxia further fuels abnormal angiogenesis and disrupts other cellular mechanisms, such as immune response [2] and cell survival [3, 4]. Thus, tumor hypoxia imaging and quantification are important in cancer research and have been an active research to search better cancer therapeutic outcomes [5–8]. There are two types of tumor hypoxia: chronic hypoxia (also known as diffusionlimited hypoxia) and acute hypoxia (also known as perfusionlimited hypoxia). Recent studies demonstrate that local tumor hypoxia behavior has profound impact in tumor metastasis and therapeutic outcomes [9, 10], hence characterizing and profiling the hypoxia in high spatiotemporal resolution can not only explore the further understanding causality between hypoxia and tumors but also is beneficial to cancer patient care.
Current in vivo preclinical diagnostic methods to determine the partial pressure of oxygen (pO_{2}) include polarographic electrode (or Eppendorf probe), photoluminescencequenching optical probe or biomarker assays based on the 2nitroimidazoles (pimonidazole and EF5). These techniques provide a direct and quantifiable measure of pO_{2} or the relative oxygen level (pO_{2} < 10 mmHg) or hypoxic fraction in tissue, but their disadvantages have limited their wide spread use. For example, the Eppendorf probe necessitates an invasive procedure (needle insertion or biopsy) and lacks spatial information. Oxygen level quantification using 2mitroimidazoles result in inconsistencies with Eppendorf probe measurements [11, 12] or with locoregional tumor control, diseasefree survival [13] and eventfree survival time [14]. PET and SPECT radiopharmaceutical tracers engineered around these biomarkers, such as ^{18}FMISO or ^{64}CuATSM, provide a noninvasive means to measure hypoxia [15, 16], and have been found to correlate with therapeutic response and outcome from radiation and chemotherapy [17, 18] when comparing average tumortomuscle ratios. However, these methods are still in the early stages of research and lack any mechanistic information causal to hypoxia.
Other approaches first quantify the hemodynamic parameters then extrapolate the local oxygen concentration. Nearinfrared spectroscopy, such as diffuse optical tomography and photoacoustics, is widely used to measure hemoglobin concentration (C_{tHb}) and its oxygen saturation (SaO_{2}) level by quantifying the differential absorption spectrum of oxy and deoxyhemoglobin molecules [19, 20]. Quantitative BOLD MRI is also capable of measuring oxygen saturation levels in vivo as demonstrated in preclinical studies [21] and have been shown to correlate to pimonidizole staining. The oxygen concentration using dynamic contrast enhanced imaging by injecting contrast agents in blood circulation to measure local vascular hemodynamics correlates to Eppendorf pO_{2} histograph and pimonidizolebased immunohistochemistry [22, 23]. Each of these techniques provides a quantifiable measure of a single factor contributing to hypoxia, such as perfusion, hemoglobin concentration, or oxygen saturation, with good spatial and temporal resolution. By combining or fusing these parameters through the implementation of oxygen transport models, the precise local pO_{2} and etiology leading to hypoxia can be investigated. Integration of mathematical modeling and imaging observations proves to be a powerful approach to understand tumor vasculature behaviors at various scales and can have application in clinical diagnosis [24–26]. The approach will become more reliable as the progression of imaging hardware provides accurate anatomical and functional measurements in high spatiotemporal resolution.
The advent of mathematical modeling in oxygen transport began as early as the twentieth century. Krogh in collaboration with Erlang, a mathematician, first approached the modeling of oxygen transport as a frame work to design experiments, interpret data, and suggest new insights on how the smallest micro vessels can supply oxygen to tissue, given the lack of technology at the time in support of his quest to understand oxygen transport in capillaries. With his model, he was able to conclude that the skeletal muscle tissue milieu was already well oxygenated and that the capillary bed only exchanged very low amount of oxygen with the muscle cells, contrary to the common belief at the time [27]. Krogh’s tissue cylindrical model set the stage for almost all subsequent models and has had tremendous and continuous impact to the field. By the 1960s, an interest in tissue oxygen transport was renewed, and steadystate and timedependent models were developed to investigate the influence of hemoglobin and myoglobin oxygen binding within the microcirculation and whole in organs systems [28]. These models expanded upon Krogh’s model to include compartments for the RBCs, the plasma layer, the capillary wall, intestinal space and cellular volume, and used to study muscle physiology [29]. For example, Hellums used these concepts of mass transport to predict the passage of RBCs through capillaries would result in pO_{2} fluctuations [30], a phenomenon only recently observed [31, 32]. Multiple parallel vessel models better accounted for the O_{2} diffusion between capillaries, where advanced numerical techniques were beginning to applied, including finite difference and finite element methods [33]. When combined with advanced computational systems, local oxygen concentrations due to tissue heterogeneity could be further investigated [33]. By 2000, Secomb, Hsu, and Pries developed a Green’s function algorithm to calculate the steadystate local pO_{2} contributed from all vessel segments within a 3D network [34, 35], and was used to study the development of microvascular networks as well as different regulatory mechanisms on blood flow in tumors [36–38]. By implementing finite difference methods, timedependent solutions of heterogeneous microvascular networks under various physiological conditions were now possible [39].
The objective of this study is to profile the 3D oxygen concentration and hypoxic fraction by fusing the multiple parameters obtained from in vivo functional imaging through the use of oxygen transport model. To obtain local oxygen concentration levels based on 3D imaging, the Krogh model has been reformulated, where the inputs are obtained from the parametric images of the vascular physiology and hemoglobin status within the tumor. Thus, a multivariate imagefusion model of pO_{2} (or MVIF model) is provided. The MVIF model depends on the spatial resolution of the imaging system, as the point spread function decreases, the voxel volume will contain a single vessel and the local pO_{2} level will be determined with higher accuracy and precision, see Fig. 1. Prior to in vivo testing, simulation studies are performed to investigate the viability of the MVIF model, where previously published biological models and microscopic data were used as a point of reference. The goals of this study are to identify an optimal voxel size and the necessary instrumental sensitivities to obtain an accurate and precise determination of pO_{2}. The range of spatial resolutions and sensitivities used in these simulation studies are consistent with in vivo dynamic contrastenhanced (DCE) imaging (clinical and preclinical MRI, CT, or photoacoustic) and optical or photoacoustic spectroscopy (PCTS). 3D tumor vasculature and hemodynamic quantification using intravital microscopy are used to simulate the in vivo parametric measurements (such as perfusion, fractional plasma volume, and the hemoglobin status within each voxel) which are subsequently fused to our model to obtain 3D pO_{2} maps. These MPO2 maps are compared on a voxelbyvoxel basis to the referenced pO_{2} values calculated by Green’s function [34]—which shows close correlation to the local tumor oxygen level using microelectrode [40]—to investigate the necessary image resolution and to determine the sensitivity by varying the statistical and systematic uncertainty in the in vivo imaging parameters.
Methods
Simulation procedure overview
The performance of our model was tested in two different tissue types: the brain and a tumor. The microvasculature within the brain served as an internal control or normal tissue, while the microvasculature of the tumor represented an abnormal or diseased tissue. The 3D microvasculature of the tumor and the brain is displayed in Fig. 2a and b, the 3D dimension of tumor encompassing entire vasculature was 0.990 × 0.810 × 0.15 mm^{3}, the dimension of brain was 0.150 × 0.160 × 0.14 mm^{3}. Basically a window chamber was employed into the dorsal flap of the animal and tumor cells were implanted subcutaneously near a vessel in the chamber to study tumorinduced angiogenesis. Intravital microscopy was used to image 3D tumor vascular structure; photometric techniques were used to quantify hemodynamic variables (such as blood flow, hematocrit) in each vessel segment of the vasculature. The detailed experimental protocol and the procedures of post image and video processing to derive blood flow and vascular branching angle can be found in the publication of Fontanella et al. [41] and Brizel et al. [42]. The Green’s function algorithms to utilize the experimental vascular inputs from window chamber model in calculating oxygen distribution were downloaded from the website [43].
In this study, the oxygen profile calculated by Green’s function was used as a reference. The Green’s function method calculates the pO_{2} at any location within the tumor by considering the contribution from all single vessel segments in the tissue volume. Once the pO_{2} profile within the entire tissue volume (brain or tumor) was completed, a virtual 3D voxel grid representing the reconstructed image volume by DCECT was superimposed onto the tissue. The average effective hemodynamic values in each finite voxel were calculated based on its known microvascular architecture. These voxelbased hemodynamic parameters are used as inputs to our singlevessel multivariate oxygen transportation model (MVIF) to calculate the pO_{2} (MPO2) in each voxel of the virtual grid. The corresponding pO_{2} (GPO2) calculated using Green’s function was also calculated and used as a reference value. A scatter plot of MPO2 versus GPO2 for each voxel was compared by performing a linear regression. Since the placement of the virtual (or imaging) voxel grid is somewhat arbitrary and depends on the voxel size, the grid was randomly translated by less than a half a voxel length for larger voxel sizes. To account for these variations and to increase the number of data points for largevoxel MPO2 to GPO2 data, the grid was translated, the new vascular architecture for each voxel extracted, and the MPO2 and GPO2 calculated and plotted.
Implementing Green’s function algorithm to calculate referened pO_{2} (GPO2)
The Green’s function algorithm developed by Hsu and Secomb [34] was used to calculate the tissue oxygen concentrations resulting from the unique microvasculature geometry and hemodynamics in each tissue. The physiological constants used in these simulations were listed in Table 1. To reduce computation time, the tissue space was first discretized into an isotropic cubic lattice, the distance between two lattice points was 15 μm in our simulation (see Fig. 3). The oxygen consumption rate at each lattice point was derived from the Michaelis–Menten equation. Similarly vessels as oxygen source were discretized into sub vessel segments with 50 μm in length. The midpoint of each sub vessel segment represented the location oxygen source. In Green’s function algorithm, the major oxygen release factors (blood flow, oxygen diffusion rate in vessel and in tissue space, hemoglobin concentration, and oxygen release rate from hemoglobin into plasma simulated by Hill’s equation) and oxygen consumption rate were considered to calculate pO_{2} at the tissue lattice point (LPO2). Although Green’s function algorithm assumes the system to be under steadystate conditions and other assumptions to reduce the computational complexity, a statistically significant correlation between the tumor oxygen consumption rate derived by Green’s function and the actual microelectrode measurements in microvasculatures was reported [40], which provides a measure of confidence in pO_{2} from Green’s function as a reference.
Once all LPO2 was determined, a virtual grid composed of isotropic finitesized voxels was superimposed onto the entire tissue, for example Fig. 3a and b demonstrated the virtual grid of 100 and 200μm voxel overlaid on tumor. The voxel pO_{2}, referred to as GPO2, was calculated by averaging all the LPO2 located inside the voxel, and represented the reference to evaluate the voxel pO_{2} by our multivariate singlevessel model.
Implementing the multivariate imagefusion (MVIF) model to calculate voxel pO_{2}(MPO2)
All MVIF algorithms were programmed in Matlab (Mathworks Inc.) A detailed derivation of the multivariate image fusion model of oxygen concentration (MVIF) is described in the Additional file 1. MVIF is a modified single cylindrical vessel model proposed by Krogh and Erlang [27, 44] used to calculate the pO_{2} in a voxel of tissue based as a function of several key physiological parameters related to oxygen supply and consumption. The final analytic equation of MVIF to calculate pO_{2} in cylindrical coordinates is:
F represents blood perfusion, \(r_{c}\) is the single vessel radius, \(r_{T}\) is the upper radial boundary in MVIF, \(pO_{2}\,(z = 0)\) is the initial pO_{2} at the entrance of the vessel, \(D\) is the oxygen diffusion constant, \(H\) is Henry’s constant, \(M\) is the oxygen consumption rate, \(m\) is the slope of the oxygenhemoglobin dissociation curve (see equation 2 in the Additional file 1), \(G_{1}\) is the geometrical term or form factor depicting radial diffusion within the voxel, and \(G_{2}\) is the geometrical term or form factor of advection along the z of cylindrical vessel.
In this simulation study, since the vasculature geometry and hemodynamic measurement inside the voxel of the virtual grid are known, some inputs for MVIF—such as the effective vessel radius \(r_{c}\), blood perfusion \(F\), and the initial pO_{2}—can be calculated precisely as they were to measure by functional imaging modalities. Hill’s equation was used twice to calculate the initial pO_{2} in each voxel in this simulation. The lumen pO_{2} in each vessel segment of the vasculature was calculated using Green’s function, the corresponding SaO_{2} in each vessel segment, therefore, can be derived using Hill’s equation. In simulation the vessel segment ID and volume contribution within each voxel were recorded, the voxel SaO_{2} from all vessel segments within the voxel was calculated using the following formula:\(\sum\limits_{i} {{\text{SaO}}_{2} (i)*{\text{vol}}(i)/V}\), \({\text{SaO}}_{2} (i)\) is the oxygen saturation of vessel segment i; \({\text{vol}}(i)\) is the volume of vessel segment i within the voxel; \(V\) is the total vascular volume of the voxel. We used Hill’s equation again to derive the initial pO_{2} as input for MVIF from this voxel SaO_{2}. The parameters or constants appearing in MVIF and Hill’s equation were listed in Table 2. The pO_{2} at any point within the voxel vessel was calculated; the average pO_{2} from the pO_{2} within the voxel represented the voxel pO_{2} calculated by MVIF, referred to as MPO2. Scattering plot of MPO2 versus GPO2 (as reference) on a voxelbyvoxel basis was plotted to evaluate the correlation and to identify the voxel outlier of which MPO2 significantly deviated from GPO2.
MVIF response to voxel size (image spatial resolution)
In general, the complexity of the vessel network depends on the voxel size and the tissue type, as illustrated in Figs. 1, 2 and 3. In functional imaging image spatial resolution is determined by the voxel size. To investigate the accuracy and precision of the MVIF model as function of the voxels sizes, linear regression analysis was used to evaluate the correlation between MPO2 and GPO2 at different voxel sizes ranging from 50 to 300 µm, in 50 µm increments. For the brain tissue, only 50 and 100 µm voxel sizes were investigated because of the size of the tissue volume, 150 µm × 160 µm × 140 µm.
Hypoxic fraction correlation
The hypoxic fraction (HF) is the fraction of the tumor volume that has a pO_{2} less than a defined threshold, which typically ranged between 2.5 and 10 mmHg. Tumor HF has been used in clinical diagnosis, and has been estimated by a variety of techniques including immunohistochemistry, computed tomography, or [^{18}F] 2fluoro2deoxyglocose PET [23, 45]. Similarly, the relationship between the HF as determined from MPO2 and GPO2 models was investigated. First, the tumor HF for MPO2 and GPO2 was calculated for various thresholds, from 2.5 to 15 mmHg in 2.5 mm steps. The number of voxels exceeding the hypoxic threshold was counted and divided by the total number of voxels in tumor. Since the brain (or normal) tissue is well oxygenated, a pO_{2} threshold ranging from 16 to 22 mmHg with 2 mmHg intervals was used.
Sensitivity and error analysis in MVIF modeling
Since nonlinear MVIF takes the hemodynamic and structural inputs from in vivo functional imaging to calculate MPO2, it is important to know (1) its response to changes in the input parameters and (2) how the hemodynamic or structural measurement error from in vivo functional imaging experiment affects the accuracy and precision of MPO2.
To answer the first objective the referenced MPO2 was calculated with the input values listed in Table 2. We then calculated MPO2 when only one input was considered as variable while other inputs remained as constant. Four new inputs which are ±10 and ±20 % from the referenced input value listed in Table 2 were used to calculate the corresponding MPO2 responses. The percent change in MPO2 compared to the referenced MPO2 value was then calculated and plotted. In this study we tested the MVIF response to following inputs: perfusion, vessel radius which is proportional to the fractional plasma volume, concentration of hemoglobin (C_{tHb}), oxygen saturation (SaO_{2}), and maximum oxygen consumption rate (M_{0}). The reference values for blood perfusion, C_{tHb}, and the SaO_{2} were selected from DCECT and PCTS measurements [46–49], and the maximum oxygen metabolic rate was chosen from the literature [50].
The second objective aims to learn how much the potential measurement error of functional DCECT could impact on the MVIF pO_{2} prediction in accuracy and precision. For this purpose we chose the voxel size equal to 150 μm because the scattering plot of GPO2 vs. MPO2 showed good correlation (see Fig. 5). Since blood perfusion and the fraction of vessel volume are two key DCECT measurements to tissue oxygenation, we evaluated the measurement error influence of those two major hemodynamic parameters to MVIF model. A Gaussian error function was used with a fullwidth at halfmaximum (FWHM) equal to 20 % of the blood perfusion to generate ten mock blood perfusions for each voxel, and then the corresponding ten MPO2 were calculated. The average of ten MPO2 and the standard error were calculated and plotted as a function of GPO2. Identical procedures were applied to the fractional vessel volume to investigate how the error in the fraction of vessel measurements from DCECT could impact the MVIF performance.
Nearestneighbor algorithm to reduce the outliers at 50μM voxel scattering plot
The 50 μm voxel size for the tumor resulted in a significant increase in the variance and deviation from a slope of 1.0 as determined from the regression analysis (see Fig. 5a). This was not observed in the normal brain microvasculature. Unlike the brain, as the voxel size decreased for the tumor, an increasing number of voxels did not include a blood vessel, included a very small section of a blood vessel, or had a neighboring voxel with a large blood vessel. To compensate for the influence of the 6neighboring voxels on a voxel’s average pO_{2} value, the average MPO2 from these surrounding voxels was added to the MPO2 value from the voxel itself to improve the correlation at 50 μm, or equivalently, to incorporate (or approximate) the boundary conditions. Therefore, the MPO2 calculation in each voxel was replaced by the average of surrounding six voxel pO_{2}.
Results
Correlation between MPO2 And GPO2 as a function of voxel size
For the normal brain microvasculature, the scatter plots of the average Green’s function pO_{2} (GPO2) and multivariate image fusion model pO_{2} (MPO2) for voxel dimensions of 50 and 100 µm were plotted in Fig. 4. At 50μm voxel, the (slope, r^{2}) values using linear regression analysis were (1.0, 0.86), at 100μm voxel, the (slope, r^{2}) were (1.0, 0.97). For the abnormal tumor microvasculature, the scatter plot and linear regression analysis for the six different voxel sizes (50–300 μm in 50 μm increment) were plotted in Fig. 5a–f. The (slope, r^{2}) using linear regression analysis at voxel sizes from 50 to 300 μm in 50 μm increment were (0.99, 0.71), (0.98, 0.80), (1.0, 0.83), (1.0, 0.75), (0.65, 0.62), and (0.3, 0.46). The corresponding Pearson correlation coefficients (R) were 0.84, 0.89, 0.86, 0.84, 0.72 and 0.67 respectively, and all correlation coefficients reached statistical significance (p < 0.05).
In Fig. 5a–c, the r^{2} value for the 50 μm voxel size was lower than that of 100 and 150 μm, which can be explained by the influence of oxygen contribution from the vessels (arterioles or venules) in the neighboring voxels. The nearest neighbor algorithm was applied to approximate this effect, where the average pO_{2} from the surrounding voxels was added to the MPO2 value and accounts voxel lacking vasculature and outliers observed in the scatter plots. After applying this algorithm, the correlation between MPO2 and GPO2 at 50 μm significantly improved (compare of Figs. 5a, 6a). The r^{2} as function of voxel size were displayed in Fig. 6b.
Hypoxic fraction correlation between MPO2 And GPO2 as function of voxel size
Hypoxia fraction (HF) of tumor is another common clinical relevance parameter to evaluate tumor oxygen level. In the brain, the pO2 threshold values were set to 16, 18, 20, and 22 mmHg; and in the tumor, the thresholds were set to 2.5–15 mmHg in 2.5 mmHg increment. Figure 7 demonstrated the normal brain HF correlation and regression analysis of GPO2 and MPO2 model; the (slope, r^{2}) for voxel size of 50 and 100 μm were (0.92, 0.97) and (0.96, 0.98) respectively. Figure 8 showed the tumor HF correlation and linear regression of voxel size 50–300 μm in 50 μm increment; the respective (slope, r^{2}) of linear regression for voxel size from 50 to 250 μm in 50 μm increment were (0.44, 0.97), (0.84, 0.98), (0.85, 0.99), (0.79, 0.94) and (0.93, 0.86).
Sensitivity of MVIF To microvascular hemodynamic and structural inputs
The changes in the local pO_{2}, either GPO2 or MPO2, due to systematic offsets in the vascular inputs are displayed in Fig. 9. Those vascular inputs were chosen based on the reported influence on tumor oxygenation [51, 52], and determined from DCECT or PCTS measurements [46–49]. These values were 10 and 20 % change in the blood vessel radius (thus, fractional vascular volume), blood perfusion, oxygen metabolic rate, oxygen saturation (SaO_{2}), and hemoglobin concentration (C_{tHb}) relative to the reference values (Table 1). The absolute fluctuation in the average MPO2 from the four vascular inputs was 9.7, 15.2, 16.0, 12.6, and 15.0 %, respectively. The oxygen consumption rate had the largest impact on tissue oxygenation, while the vessel radius (or the fractional vascular volume) had the lowest impact on tissue oxygenation.
MVIF response to the measurement error of microvascular inputs
To investigate how the precision of the measurement using in vivo functional imaging modality (e.g. DCECT) influence the MPO2 accuracy and precision, a Gaussian error function was used to generate ten configurations of perturbed maps of blood perfusions fractional vessel volume and the MPO2 and GPO2 maps calculated. The full width at half maximum (FWHM) of the Gaussian error function was set to 20 % of the mean vascular input value. The variation in MPO2 due to the measurement error in perfusion for the 150 μm voxel size is shown in Fig. 10a, where the error bar represents the standard deviation from these ten simulations. Similarly, the MPO2 variation due to the measurement error in the fractional vessel volume is shown in Fig. 10b. The Coefficient of variation (CV) is used to quantify the dispersion of the data relative to the mean. An average CV of the MPO2 as a result of the measurement error in blood perfusion and the fraction of vessel volume was 6.4 and 7.0 %.
Discussion
Many preclinical and clinical cancer investigations suggest that two types of hypoxia occur heterogeneously within a solid tumor: acute hypoxia (cycling hypoxia) and chronic hypoxia (diffusionlimited hypoxia) [10, 53]. In several tumor model acute hypoxia promotes tumor angiogenesis and tumor metastasis [10, 54], hence determining the etiology of hypoxia can provide new insights into predicting therapeutic response and developing novel therapeutic protocols to enhance efficacy. Here we proposed a novel assay to delineate diffusion and perfusionbased hypoxia based on insufficient vasculature related to (G_{1} and D, the geometric diffusion length and rate, respectively) and poorly blood perfused tissue related to (G_{2} and F, the geometry related to convective forces and perfusion) under a steadystate conditions (see equation 3 and 4 in Supplement Data). By considering the variation of these parameters as a function of time [e.g., Perfusion = Perfusion(t) and m = m(t)], acute and chronic hypoxia could be assessed, which could be tested relative to variations in angiogenic (VEGF, FGF, etc.) and inflammatory (IL6, histamine, prostaglandins, NO) activity or their corresponding therapies. As an initial step, an in vivo highresolution oxygen profiling assay is being proposed to image the spatial variations in tumor hypoxia. This capability will further advance our understanding the role hypoxia has in solid tumors as well as in developing new cancer treatments, such as in antiangiogenic therapy.
In this study, a method was proposed that fuses microvascular functional attributes from functional imaging modalities through a multivariate oxygen transport model to obtain local tumor oxygen levels was investigated. Highresolution DCECT (or DCEPCT) and PCTS can longitudinally characterize local vessel structure and hemodynamics as well as tumor metabolic status. Those measurements represent tumor oxygenation status thus in principle a biophysical oxygen transportation model, in this case a multivariate modified Krogh model for a finite volume, can take the real measurements as inputs to calculate local oxygen level, and furthermore to profile tumor oxygen status. The major challenge to verify the model prediction is to have simultaneous tumor functional measurements and corresponding oxygen level measurement in the finite volume. To the best of our knowledge, no such experiment or data has been conducted or published. To evaluate this idea and our multivariate model, we used the well characterized tumor or brain microvasculature and functions using intravital confocal microscopy, and Secomb’s 3D oxygen transportation model to calculate the pO_{2} distribution as a reference to evaluate the voxel pO_{2} from MVIF model. The tumor oxygen consumption rates derived from Secomb’s 3D model agree closely with the oxygen electrode probe measurements [40]. A major limitation of this study is the limited photon penetration from confocal microscopy, thus the simulation results from this study would only represent the peripheral microvasculature or microvasculature grown in window chamber [55, 56], which could be different from the microvasculature in other region of tumor. A second constraint of this investigation was the lack of few key measurements, such as the oxygen consumption rate, thus in simulation they were either derived from appropriated biophysical equation or assigned as constant.
As depicted in Fig. 1, the voxel size is associated with the vascular complexity or average inter vessel spacing and can have a significant impact on the accuracy and precision of the multivariate imagefusion algorithm (MVIF) model. An ideal model would provide a scatter plot with a flat r^{2} and a slope of 1.0 for all voxel sizes. As shown in Fig. 5b, this is clearly not the case, where an optimal voxel size was observed for the tumor and potentially the brain. Visually, this appears to depend on the voxel size relative to the inter vessel spacing or vascular density (see Fig. 3). For voxel sizes ranging from 100 to 200 μm, the coefficient of determination (r^{2}), reached a maximum and remained relatively flat. For relatively small voxel sizes (50 μm), the average oxygen diffusion length and inter vessel spacing can exceed the voxel’s dimensions. As a result, two outlier groups were introduced into the scatter plot of MPO2 versus GPO2 for the tumor: an overestimated group, of which MPO2 was exceedingly greater than GPO2, and the underestimated group. Since these outliers were not observed for the 50 µm voxel data in the normal brain tissue, it demonstrates the impact of the abnormal and heterogeneous structure and function of the tumor vasculature on these results. To correct for these outliers, an algorithm was developed to account for oxygen diffusion from neighboring voxels (Fig. 6). For relatively larger voxel sizes, the precision and accuracy of MPO2 became worse and the slope (thus sensitivity) decreased; thus, the single vessel model can no longer adequately represent the complexity or heterogeneity of the vasculature, and as a result, the uncertainty in the average pO_{2} in a voxel becomes unacceptable. Given that the inter vessel spacing ranged from ~12 to 125 μm (Fig. 3), consistent with other tumor models (K, L, M), and was acquired within the periphery or rim of the tumor (Fig. 2), the results from this study show that the proposed modified Krogh image fusion model is accurate and precise for voxel sizes 200 μm and below (r^{2} < 0.75 and slope < 0.98). Therefore, the spatial resolution needed will need to be 200 μm or less. Such resolution can be obtained by many small animal imaging systems (photoacoustic, microCT, microMRI).
The hypoxic fraction (HF) indicates the hypoxic status of the entire tumor, a parameter used in 2nitroimidazole based immunohistochemistry. Figure 7 showed the HF correlation of MPO2 and the referenced GPO2 with thresholds at 16, 18, 20, and 22 mmHg, a close regression was observed which shows that MVIF can accurately and precisely predict HF as a result of the normal microvasculature. In Fig. 8, the tumor HF data with threshold from 2.5 to 15.0 mmHg with 2.5 mmHg increment were linearly distributed; the linear regression analysis showed that the r^{2} at all voxel sizes was significant except at 300 µm albeit the HF from MVIF was consistently lower than that from Green’s function, and the regression offset was higher than that of brain microvasculature. Abnormal tumor microvessel structure or hemodynamics or both contributed to the HF offset and accuracy.
The oxygen metabolic rate, the blood flow perfusion, and hemoglobin concentration were three dominant factors in tissue oxygen transportation, as displayed in Fig. 9. Although the direct hemoglobin measurements and oxygen metabolic rates were not available in this simulation investigation, we chose Hill’s equation and Michaelis–Menton equation to estimate the hemoglobin concentration and oxygen metabolic rate in MPO2 calculation. For future in vivo experiments monitoring tumor pO2 fluctuations as function of space and time, all three parameters should be measured to achieve accurate and precise MPO2 estimation using MVIF. PCTS is capable to derive hemoglobin concentration and oxygen saturation in high spatiotemporal resolution, the oxygen consumption rate can be derived from the fraction of cell volume from DCECT or dynamic contrast enhanced photoacoustic tomography. The use of photoacoustic imaging alone can avoid coregistration with DCECT, and the concern of radiation superimposing on the tumor progression or compound treatment.
The influence of measurement error of functional imaging to the MPO2 precision and accuracy was simulated and summarized in Fig. 10. Overall, 20 % error (FWHM) in perfusion or fractional vessel volume did not deteriorate accuracy and precision when at least 10 measurements were acquired at each voxel and used to estimate the pO_{2}.
There remains limitations of this technique as well as some potential future directions. A key limitation of the proposed technique is for larger voxel sizes. If a model can be devised to rescue the MPO2 versus GPO2 correlation beyond 200 μm, the ability to translate into the clinic is viable.
Multivessel models consisting of 2 and 3 parallel cylindrical vessels with identical dimensions and hemodynamics and uniformly spaced within 250 and 300 µm voxels were simulated. However, the improvement was limited. Introducing symmetry into these models and simple bifurcated structures could explain the scatter and nonlinearity in the data; however, identifying or imposing a single concept or methodology would challenging, and requires additional constraints, such as including angiogenic information or inferring a scaling factor based on fractals [57, 58]. Additional pathological features affecting oxygen transport should also be considered, such as oxygen permeability across the vessel wall. Even though tumor vasculature is highly fenestrated and the pressure gradient across the vessel wall reduced due to elevated interstitial fluid pressure, models including oxygen permeability suggest this may have a nonnegligible effect [59, 60]. With the ability to measure the permeabilitysurface area product and interstitial fluid pressure through in vivo imaging, it may be possible to test these models [46, 61]. Green’s function solution of oxygen transport has a number of advantages in the way it handles boundary conditions, the ability to handle a larger set of physiological parameters, efficiency of calculation, and validation to in vivo measurements, it lacks the ability to handle necessary advanced features FDTD and FEM methods support, such as dynamic changes in its parameters and oxygen permeability.
Conclusion
The results from this simulation study demonstrate that the fusion of in vivo functional imaging based on the MPO2 model to quantify local tumor oxygen concentrations is feasible. A significant correlation was measured between the MPO2 model, a single vessel model, and the Green’s function algorithm (GPO2), a detailed microvascular model, for voxel sizes ranged from 50 to 200 μm, where MPO2 was calculated based on in vivo functional imaging measurements. This upper limit is consistent with the spatial resolution from existing small animal scanners, and provides a new technique to assay in vivo intratumor hypoxia. Future work will investigate the potential to monitor the dynamic changes in pO_{2}. This additional capability will be able to characterize regions of the tumor undergoing chronic and acute forms of hypoxia and the hemodynamics parameters responsible, thus providing critical information on the role hypoxia and metabolism play in cancer progression and therapy, in particular antiangiogenic therapies [10, 62].
Abbreviations
 DCECT:

dynamic contrastenhanced computed tomography
 PCTS:

photoacoustic computed tomographic spectroscopy
 pO_{2} :

oxygen partial pressure in mmHg
 C_{tHb} :

hemoglobin concentration
 SaO_{2} :

oxygen saturation
 GPO2:

average pO_{2} derived in a finite volume using Green’s function method
 MVIF:

multivariate image–fusion algorithm
 MPO2:

average pO_{2} derived in a finite volume using MVIF model
 Rsq or r^{2} :

Rsquared value
References
 1.
Jain RK. Normalization of tumor vasculature: an emerging concept in antiangiogenic therapy. Science. 2005;307(5706):58–62.
 2.
Barsoum IB, et al. A mechanism of hypoxiamediated escape from adaptive immunity in cancer cells. Cancer Res. 2014;74(3):665–74.
 3.
Huang Y, et al. Vascular normalization as an emerging strategy to enhance cancer immunotherapy. Cancer Res. 2013;73(10):2943–8.
 4.
Coussens LM, Zitvogel L, Palucka AK. Neutralizing tumorpromoting chronic inflammation: a magic bullet? Science. 2013;339(6117):286–91.
 5.
Semenza GL. Hypoxiainducible factors: mediators of cancer progression and targets for cancer therapy. Trends Pharmacol Sci. 2012;33(4):207–14.
 6.
Hendrickson K, et al. Hypoxia imaging with [F18] FMISOPET in head and neck cancer: potential for guiding intensity modulated radiation therapy in overcoming hypoxiainduced treatment resistance. Radiother Oncol. 2011;101(3):369–75.
 7.
Bell C, et al. Hypoxia imaging in gliomas with 18Ffluoromisonidazole PET: toward clinical translation. Semin Nucl Med. 2015;45(2):136–50.
 8.
Cao N, et al. Monitoring the effects of antiangiogenesis on the radiation sensitivity of pancreatic cancer xenografts using dynamic contrastenhanced computed tomography. Int J Radiat Oncol Biol Phys. 2014;88(2):412–8.
 9.
Wilson WR, Hay MP. Targeting hypoxia in cancer therapy. Nat Rev Cancer. 2011;11(6):393–410.
 10.
Rofstad EK, et al. Tumors exposed to acute cyclic hypoxic stress show enhanced angiogenesis, perfusion and metastatic dissemination. Int J Cancer. 2010;127(7):1535–46.
 11.
Nordsmark M, et al. Measurements of hypoxia using pimonidazole and polarographic oxygensensitive electrodes in human cervix carcinomas. Radiother Oncol. 2003;67(1):35–44.
 12.
Evans SM, et al. Comparative measurements of hypoxia in human brain tumors using needle electrodes and EF5 binding. Cancer Res. 2004;64(5):1886–92.
 13.
Kaanders JH, et al. Pimonidazole binding and tumor vascularity predict for treatment outcome in head and neck cancer. Cancer Res. 2002;62(23):7066–74.
 14.
Evans SM, et al. Patterns and levels of hypoxia in head and neck squamous cell carcinomas and their relationship to patient outcome. Int J Radiat Oncol Biol Phys. 2007;69(4):1024–31.
 15.
Mees G, et al. Molecular imaging of hypoxia with radiolabelled agents. Eur J Nucl Med Mol Imaging. 2009;36(10):1674–86.
 16.
Troost EG, et al. Correlation of [18F]FMISO autoradiography and pimonidazole [corrected] immunohistochemistry in human head and neck carcinoma xenografts. Eur J Nucl Med Mol Imaging. 2008;35(10):1803–11.
 17.
Matsumoto K, et al. The influence of tumor oxygenation on hypoxia imaging in murine squamous cell carcinoma using [64Cu]CuATSM or [18F]Fluoromisonidazole positron emission tomography. Int J Oncol. 2007;30(4):873–81.
 18.
Padhani AR, et al. Imaging oxygenation of human tumours. Eur Radiol. 2007;17(4):861–72.
 19.
Yalowitz JA, et al. Cytotoxicity and cellular differentiation activity of methylenebis(phosphonate) analogs of tiazofurin and mycophenolic acid adenine dinucleotide in human cancer cell lines. Cancer Lett. 2002;181(1):31–8.
 20.
Bayer CL, Luke GP, Emelianov SY. Photoacoustic imaging for medical diagnostics. Acoust Today. 2012;8(4):15–23.
 21.
Christen T, et al. Tissue oxygen saturation mapping with magnetic resonance imaging. J Cereb Blood Flow Metab. 2014;34(9):1550–7.
 22.
Cooper RA, et al. Tumour oxygenation levels correlate with dynamic contrastenhanced magnetic resonance imaging parameters in carcinoma of the cervix. Radiother Oncol. 2000;57(1):53–9.
 23.
Gulliksrud K, et al. Quantitative assessment of hypoxia in melanoma xenografts by dynamic contrastenhanced magnetic resonance imaging: intradermal versus intramuscular tumors. Radiother Oncol. 2010;97(2):233–8.
 24.
Kim E, et al. Multiscale imaging and computational modeling of blood flow in the tumor vasculature. Ann Biomed Eng. 2012;40(11):2425–41.
 25.
Stamatelos SK, et al. A bioimage informatics based reconstruction of breast tumor microvasculature with computational blood flow predictions. Microvasc Res. 2014;91:8–21.
 26.
TomaDasu I, Dasu A, Brahme A. Quantifying tumour hypoxia by PET imaging—a theoretical analysis. Adv Exp Med Biol. 2009;645:267–72.
 27.
Krogh A. The number and distribution of capillaries in muscles with calculations of the oxygen pressure head necessary for supplying the tissue. J Physiol. 1919;52(6):409–15.
 28.
Popel AS. Theory of oxygen transport to tissue. Crit Rev Biomed Eng. 1989;17(3):257–321.
 29.
Eggleton CD, et al. Calculations of intracapillary oxygen tension distributions in muscle. Math Biosci. 2000;167(2):123–43.
 30.
Hellums JD. The resistance to oxygen transport in the capillaries relative to that in the surrounding tissue. Microvasc Res. 1977;13(1):131–6.
 31.
Golub AS, Pittman RN. Erythrocyteassociated transients in PO2 revealed in capillaries of rat mesentery. Am J Physiol Heart Circ Physiol. 2005;288(6):H2735–43.
 32.
Barker MC, Golub AS, Pittman RN. Erythrocyteassociated transients in capillary PO2: an isovolemic hemodilution study in the rat spinotrapezius muscle. Am J Physiol Heart Circ Physiol. 2007;292(5):H2540–9.
 33.
Popel AS, Charny CK, Dvinsky AS. Effect of heterogeneous oxygen delivery on the oxygen distribution in skeletal muscle. Math Biosci. 1986;81(1):91–113.
 34.
Secomb TW, et al. Green’s function methods for analysis of oxygen delivery to tissue by microvascular networks. Ann Biomed Eng. 2004;32(11):1519–29.
 35.
Secomb TW, et al. Theoretical simulation of oxygen transport to brain by networks of microvessels: effects of oxygen supply and demand on tissue hypoxia. Microcirculation. 2000;7(4):237–47.
 36.
Secomb TW, et al. Analysis of oxygen transport to tumor tissue by microvascular networks. Int J Radiat Oncol Biol Phys. 1993;25(3):481–9.
 37.
Secomb TW. Theoretical models for regulation of blood flow. Microcirculation. 2008;15(8):765–75.
 38.
Pries AR, et al. The shunt problem: control of functional shunting in normal and tumour vasculature. Nat Rev Cancer. 2010;10(8):587–93.
 39.
Goldman D, Popel AS. A computational study of the effect of capillary network anastomoses and tortuosity on oxygen transport. J Theor Biol. 2000;206(2):181–94.
 40.
Dewhirst MW, et al. Determination of local oxygen consumption rates in tumors. Cancer Res. 1994;54(13):3333–6.
 41.
Fontanella AN, et al. Quantitative mapping of hemodynamics in the lung, brain, and dorsal window chambergrown tumors using a novel, automated algorithm. Microcirculation. 2013;20:724–35.
 42.
Brizel DM, et al. A comparison of tumor and normal tissue microvascular hematocrits and red cell fluxes in a rat window chamber model. Int J Radiat Oncol Biol Phys. 1993;25(2):269–76.
 43.
Secomb TW. http://physiology.arizona.edu/people/secomb/network. Accessed on May 26 2011.
 44.
Krogh A. The rate of diffusion of gases through animal tissues, with some remarks on the coefficient of invasion. J Physiol. 1919;52(6):391–408.
 45.
Komar G, et al. 18FEF5: a new PET tracer for imaging hypoxia in head and neck cancer. J Nucl Med. 2008;49(12):1944–51.
 46.
Cao M, et al. Developing DCECT to quantify intratumor heterogeneity in breast tumors with differing angiogenic phenotype. IEEE Trans Med Imaging. 2009;28(6):861–71.
 47.
Krishnamurthi G, et al. Functional imaging in small animals using Xray computed tomography–study of physiologic measurement reproducibility. IEEE Trans Med Imaging. 2005;24(7):832–43.
 48.
Stantz KM, Liang Y, Hutchins GD. Kinematic modeling and its implication in longitudinal chemotherapy study of tumor physiology: ovarian xenograft mouse model and contrastenhanced dynamic CT. Proc SPIE. 2004;5369:769–79.
 49.
Stantz KM, et al. Photoacoustic spectroscopic imaging of intratumor heterogeneity and molecular identification. Proc SPIE BIOS. 2006;6086:36–47.
 50.
Arthur C, Guyton JEH. Textbook of medical physiology. Philadelphia: Elsevier Saunders; 2006.
 51.
Batchelor TT, et al. Improved tumor oxygenation and survival in glioblastoma patients who show increased blood perfusion after cediranib and chemoradiation. Proc Natl Acad Sci USA. 2013;110(47):19059–64.
 52.
Stylianopoulos T, Jain RK. Combining two strategies to improve perfusion and drug delivery in solid tumors. Proc Natl Acad Sci USA. 2013;110(46):18632–7.
 53.
Palmer GM, et al. Optical imaging of tumor hypoxia dynamics. J Biomed Opt. 2010;15(6):066021.
 54.
Rofstad EK, et al. Fluctuating and diffusionlimited hypoxia in hypoxiainduced metastasis. Clin Cancer Res. 2007;13(7):1971–8.
 55.
Palmer GM, et al. In vivo optical molecular imaging and analysis in mice using dorsal window chamber models applied to hypoxia, vasculature and fluorescent reporters. Nat Protoc. 2011;6(9):1355–66.
 56.
Papenfuss HD, et al. A transparent access chamber for the rat dorsal skin fold. Microvasc Res. 1979;18(3):311–8.
 57.
Gazit Y, et al. Fractal characteristics of tumor vascular architecture during tumor growth and regression. Microcirculation. 1997;4(4):395–402.
 58.
Baish JW, Jain RK. Fractals and cancer. Cancer Res. 2000;60(14):3683–8.
 59.
Skeldon AC, et al. Modelling and detecting tumour oxygenation levels. PLoS ONE. 2012;7(6):e38597.
 60.
Barrett MJ, Suresh V. Extra permeability is required to model dynamic oxygen measurements: evidence for functional recruitment? J Cereb Blood Flow Metab. 2013;33(9):1402–11.
 61.
Hompland T, et al. Assessment of the interstitial fluid pressure of tumors by dynamic contrastenhanced magnetic resonance imaging with contrast agents of different molecular weights. Acta Oncol. 2013;52(3):627–35.
 62.
Cairns RA, Hill RP. Acute hypoxia enhances spontaneous lymph node metastasis in an orthotopic murine model of human cervical carcinoma. Cancer Res. 2004;64(6):2054–61.
 63.
Grote J, Susskind R, Vaupel P. Oxygen diffusivity in tumor tissue (DScarcinosarcoma) under temperature conditions within the range of 20–40 degrees C. Pflugers Arch. 1977;372(1):37–42.
 64.
Zander R. Cellular oxygen concentration. Adv Exp Med Biol. 1975;75:463–7.
 65.
Fournier RL. Basic transport phenomena in biomedical engineering. 3rd ed. Boca Raton: CRC Press; 2011.
Authors’ contributions
KMS carried out the idea in fusing mathematical models and in vivo functional imaging to estimate entire 3D oxygen distribution in tumor; CWL carried out simulation programming and evaluation using oxygen profile from Green’s function as a standard. All authors read and approved the final manuscript.
Acknowledgements
The first author would like to give thanks to the support from previous employer: Eli Lilly and Company, and Covance. The first author also would like give thanks to the support from School of Health Sciences at Purdue University in West Lafayette IN.
Competing interests
The authors declare that they have no competing interests.
Availability of data and materials
The datasets during and/or analysed during the current study available from the corresponding author on reasonable request.
Funding
NIH/NIBIB R21 EB012849, PI: Stantz KM.
Author information
Affiliations
Corresponding author
Additional file
Additional file 1.
Additional data.
Rights and permissions
Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The Creative Commons Public Domain Dedication waiver (http://creativecommons.org/publicdomain/zero/1.0/) applies to the data made available in this article, unless otherwise stated.
About this article
Cite this article
Lee, CW., Stantz, K.M. Development of a mathematical model to estimate intratumor oxygen concentrations through multiparametric imaging. BioMed Eng OnLine 15, 114 (2016). https://doi.org/10.1186/s1293801602355
Received:
Accepted:
Published:
DOI: https://doi.org/10.1186/s1293801602355
Keywords
 Multivariate Krogh model
 In vivo functional imaging
 Dynamic contrast enhanced computed tomography
 Photoacoustic spectroscopy