- Open Access
Kinetic modeling of tumor growth and dissemination in the craniospinal axis: implications for craniospinal irradiation
Radiation Oncologyvolume 1, Article number: 48 (2006)
Medulloblastoma and other types of tumors that gain access to the cerebrospinal fluid can spread throughout the craniospinal axis. The purpose of this study was to devise a simple multi-compartment kinetic model using established tumor cell growth and treatment sensitivity parameters to model the complications of this spread as well as the impact of treatment with craniospinal radiotherapy.
A two-compartment mathematical model was constructed. Rate constants were derived from previously published work and the model used to predict outcomes for various clinical scenarios.
The model is simple and with the use of known and estimated clinical parameters is consistent with known clinical outcomes. Treatment outcomes are critically dependent upon the duration of the treatment break and the radiosensitivity of the tumor. Cross-plot analyses serve as an estimate of likelihood of cure as a function of these and other factors.
The model accurately describes known clinical outcomes for patients with medulloblastoma. It can help guide treatment decisions for radiation oncologists treating patients with this disease. Incorporation of other treatment modalities, such as chemotherapy, that enhance radiation sensitivity and/or reduce tumor burden, are predicted to significantly increase the probability of cure.
Medulloblastoma is a relatively common primary tumor of the central nervous system (CNS) in the pediatric population, representing about 20% of brain tumors in this group . The mainstays of treatment include maximal surgical resection followed by chemotherapy and radiation to the entire craniospinal axis (brain and spine), also known as craniospinal irradiation (CSI) . Radiotherapists treat the entire craniospinal axis because the tumor cells have direct axis to the subarachnoid space, and, hence, the cerebrospinal fluid (CSF), which can provide a route for metastatic spread throughout the craniospinal axis. Early clinical studies indicated the importance of full CSI as opposed to treatment of smaller, gross-tumor-directed volumes . Various clinical trials have been performed or are underway to study reduction of the radiation dose and attendant complications of CSI, possibly by way of intensifying chemotherapy. Nonetheless, CSI has retained its role as a critical component in the multimodality management of medulloblastoma [4, 5].
Other primary and metastatic tumors of the CNS can also spread throughout the craniospinal axis via the CSF with leptomeningeal carcinomatosis, a descriptive term for tumor studding along the leptomeninges. In such patients, CSI may play a palliative role in the treatment armamentarium . These patients are occasionally treated with intrathecal chemotherapy, which is another means of treating the entire subarachnoid space [7, 8].
Delivery of CSI with standard photon therapy presents a geometric dilemma that is typically solved by the use of opposed lateral brain fields that are matched with collimator and treatment couch rotations to one or two posterior-anterior spine fields (Figure 1, reprinted with permission). When photons (as opposed to protons or electrons) are used to deliver CSI, these field arrangements ultimately lead to irradiation of a large portion of a patient's normal tissues, including the vertebral bodies with their productive bone marrow, as well as the viscera of the thorax, abdomen, and pelvis. Complications during treatment can include nausea, esophagitis, diarrhea and life-threatening myelosuppression (particularly in patients who have undergone preceding courses of chemotherapy); long-term complications may involve growth disturbances, hypothyroidism, and, especially in children, induction of second malignancies [9, 10].
By the nature of their arrangement, the treatment fields described above functionally compartmentalize the craniospinal axis into 'brain' and 'spine' compartments. Because of acute treatment-related toxicities, especially myelosuppression (a complication that can arise early in the treatment course), it is occasionally necessary to suspend treatment of the spine temporarily while treatment of the brain continues. Since the brain and spine are in communication via the cerebrospinal fluid, holding treatment in one compartment may threaten tumor control in the other secondary to seeding of cells between these compartments. For example, tumor regrowth in the spine that occurs during treatment delays can seed tumor cells into the brain. CSF flow between the brain and spine may be considered analogous to the problem of a primary extracranial tumor forming distant metastases via hematogenous spread. Previous reports have modeled the process of metastasis, with the ultimate goal of evaluating and optimizing therapeutic intervention within the contexts of these models .
In this report we describe a kinetic model of tumor transport in the craniospinal axis (subarachnoid space and ventricle spaces) for medulloblastoma. The model is tested to assess if it can reasonably describe established clinical observations. Following this, the relative effects of changes in parameters incorporated in the model, such as those associated tumor cell shedding and adhesion, are discussed.
The craniospinal axis is considered as having two tissue compartments, brain (b) and spine (s), with two phases, solid tumor (t) and cerebrospinal fluid (f), within each compartment (Figure 2). In the model the brain is not subdivided into supratentorial and posterior fossa (where medulloblastomas arise) compartments but rather as a single compartment. Recognizing that CSF flow is temporally and spatially heterogeneous , we assume that each fluid phase is well-mixed, as a crude approximation. Between the two compartments, cell transfer is governed by the volumetric flow rate, Qf, and the cell concentration in the fluid phases, i.e., the number of cells in the fluid phase divided by the volume of that phase. This is a reasonable assumption since the CSF flows relatively freely between the brain and spine compartments. Within each tissue compartment, transfer of cells between the phases is determined by the rate of adhesion of cells from the fluid phase onto the solid phase and by the rate of shedding of cells from the solid phase into the fluid phase. We assume that adhesion and shedding are described by the product of cell number and the rate constants kadh and kshed, respectively. However, not all of the cells shed into the fluid phase will be viable, and adhesion will account for only a portion of the cells cleared from the CSF. This is accounted for in the model by incorporating modulating efficiency factors for transfer of viable cells from the CSF to solid tumor and from solid tumor to CSF, γf and γt, respectively, which range in value from 0 to 1.
Finally, the tumor cell growth rate in each phase is assumed to be a linear function of tumor cell number (first-order growth kinetics), i.e., the product of growth rate constant, and cell number for that compartment and phase. For the purposes of this model, we are interested in estimating tumor control and focus on the development of relatively small tumors. Thus, we can ignore substrate and transport limitations that would require Gompertzian-type models of tumor growth . Of course, much more complex growth models could be employed in this model, using the numerical solution technique described below.
Based on the above assumptions and in the absence of radiation-induced cell killing, the following system of ordinary differential equations is derived:
(1)dNs,f/dt = kg,fNs,f + Qf(Nb,f/Vb - Ns,f/Vs) + γtkshedNs,t - kadhNs,f
(2)dNs,t/dt = kg,tNs,t - kshedNs,t + γfkadhNs,f
(3)dNb,f/dt = kg,fNb,f + Qf(Ns,f/Vs - Nb,f/Vb) + γtkshedNb,t - kadhNb,f
(4)dNb,t/dt = kg,tNb,t - kshedNb,t + γfkadhNb,f,
where Nx,y is the number of cells in compartment x, phase y; kg,y is the growth rate constant in phase y; and Vs and Vb are the volumes of the spine and brain subarachnoid space compartments, respectively. 's' refers to spine, 'b' refers to brain, 'f' refers to fluid, and 't' refers to tumor.
Rate constants in the model have been derived from in vivo data when possible so as to reflect clinical reality as closely as possible. Baseline values for these parameters are listed in Table 1. The value of kg,t used in the scenarios described in the results section (0.01 hr-1) is within the range of values that can be derived from the medulloblastoma potential doubling times (Tpot) of 25 to 82 hours described in the work of Ito et al .
The study by Ito et al also reported an observed clinical doubling time of 480–576 hours. Since there is, currently, no direct way of establishing kshed, we have estimated its value. By assuming that the discrepancy between Tpot and observed doubling times is due solely to cells shedding from the tumor (and not from, for example, cell growth slowing with increasing tumor size nor from host immunologic attack of the tumor), we can establish an upper limit value for kshed; this value is close to 0.01 hr-1. Since this value for kshed has to be a gross overestimate (the other factors mentioned above do indeed contribute to the discrepancy between Tpot and the observed doubling time), we have initially, arbitrarily, set it to a value that may be more in line with clinical reality, on the order of 0.001 hr-1. We have taken kadh to be 10% of the value of kshed (0.0001 hr-1), again as a rough estimate, with the assumption that it is more difficult for cells to adhere to other cells when they are flowing in the CSF. The values for kshed and kadh are both modulated by the values γf and γt, as described above.
The value for Qf, the volumetric flow rate and the spine and brain CSF volumes are taken from Bergsneider . The values used for the volumes of the brain and spine CSF spaces are rough averages between what would be expected in a child and in an adult.
The system of equations can be discretized and re-arranged to yield the cell number at time i+1 as a function of the cell numbers at time i, yielding the following system of new equations:
(5) Ns,f,i+1 = Ns,f,i + Δt(kg,fNs,f,i + Qf(Nb,f,i/Vb - Ns,f,i/Vs) + γtkshedNs,t,i - kadhNs,f,i
(6) Ns,t,i+1 = Ns,t,i + Δt(kg,tNs,t,i -kshedNs,t,i + γfkadhNs,f,i)
(7) Nb,f,i+1 = Nb,f,i + Δt(kg,fNb,f,i + Qf(Ns,f,i/Vs - Nb,f,i/Vb) + γtkshedNb,t,i - kadhNb,f,i)
(8) Nb,t,i+1 = Nb,t,i + Δt(kg,tNb,t,i - kshedNb,t,i + γfkadhNb,f,i)
We then consider the situation in which a dose of radiation, D, is applied to a compartment over a short period of time, immediately prior to time i+1. We assume that D instantaneously reduces the number of cells capable of reproducing by a factor of . D0 is a parameter traditionally used to describe radiosensitivity and represents the dose required to reduce a clonogenic cell population to (ln 2)-1, or about 37%, of its initial value . The D0 value ranged from 130 to 153 cGy for three cultured medulloblastoma cell lines studied in vitro, with a minimal shoulder to the curves as evidenced by the low extrapolation value of about 1.5 .
At time i+1 immediately following a dose of radiation, we can modify the above system of equations to yield:
(9) Ns,f,i+1 = [Ns,f,i + Δt(kg,fNs,f,i+Qf(Nb,f,i/Vb-Ns,f,i/Vs)+ γtkshedNs,t,i-kadhNs,f,i)]
(10) Ns,t,i+1 = [Ns,t,i + Δt(kg,tNs,t,i-kshedNs,t,i+γfkadhNs,f,i)]
(11) Nb,f,i+1 = [Nb,f,i + Δt(kg,fNb,f,i+Qf(Ns,f,i/Vs-Nb,f,i/Vb)+ γtkshedNb,t,i-kadhNb,f,i)]
(12) Nb,t,i+1 = [Nb,t,i + Δt(kg,tNb,t,i-kshedNb,t,i+γfkadhNb,f,i)]
where Ds and Db are the doses administered in a single fraction to the spinal and brain compartments, respectively.
The equations were employed to numerically model various clinical scenarios, with adjustments made in different scenarios for the rate constants and for D0. Cell growth was not allowed in compartment i (i.e., kg,i was set to zero) if the number of cells N was less than 0.05, since it is at that point that the Poisson distribution, e-N, yields a tumor control probability of about 95%. Since we have not incorporated the effects of chemotherapy, a prescribed dose of 54 Gy to the brain and 36 Gy to the spine, administered at 1.8 Gy per day, has been used. This is the standard treatment regimen for a patient with medulloblastoma who is free from clinical evidence of disease outside the brain and negative CSF cytology . Note that the model in its current formulation does not directly incorporate the effects of chemotherapy, which has emerged as a central component of therapy for patients with medulloblastoma. Chemotherapy may improve radisoensitvity, in addition to direct cytotoxic action on the tumor, improving outcome, as discussed below.
In all of the clinical scenarios, we have set Nb,t to be 1 × 109 cells, roughly equal to the number of cells in one cm3 of tumor, at t = 0. We have set N to be equal to 1, initially, in all other phases. Parameters for the initial set of scenarios are listed in Table 1.
In this scenario (Figure 3), results following a standard course of treatment for the model allowing for flow (Qf = 25 ml/hr) and not allowing for flow (Qf = 0) are shown. Cure is achieved in both settings. This fits clinical experience; 54 Gy of radiation to the brain/posterior fossa and 36 Gy to the spine has a high probability of curing medulloblastoma. By adjusting various parameters such as kg and D0, it is obvious that differing outcomes would be observed. For example, if a patient's medulloblastoma cells were more radioresistant (i.e., had a higher D0 value), the outcome would not be as favorable. This is further discussed in scenario IV. Scenario I also shows that when flow between the spine and brain compartments is allowed there is a rapid rise in Ns,t and Ns,f.
In this scenario II (Figure 4), results following the introduction of a 3-week break in the spine portion of the treatment are described. As described above, such breaks may be necessitated when the acute reactions of the spine portion of CSI become life-threatening. The deleterious impact of treatment delay on outcomes in medulloblastoma has been documented in several retrospective series [18–20]. The kinetic model recapitulates this finding. In Figure 4a (with Qf = 25 ml/hr), the introduction of the break prevents sterilization of the spine phases, which were nearing sterilization just prior to the break. Enough cells remain to eventually repopulate all phases in the model. In a version of the model not allowing for flow (Qf = 0), shown in Figure 4b, the break never becomes an issue for cure because the spine is never seeded with cells from the brain. The brain compartment is easily sterilized with 54 Gy.
In this scenario (Figure 5), the importance of the parameter values in the model results is illustrated. Using the same scenario details as in scenario II, we have lowered the value for kshed and kadh by one order of magnitude each. This scenario models the response of tumors that are 'stickier' than those in the previous scenarios. Despite a three-week break, tumor control is nonetheless achieved. The reason is clear by comparison with Figure 5. By the time that the break is instituted, the value of N in the solid and fluid spine phases is significantly lower than in the previous scenario; seeding from the brain did not occur to the same extent since the cancer cells were less likely to be shed into the CSF.
In this scenario (Figure 6), the importance of the value of D0 is shown. We have used the original parameters as in scenario I, but increased the D0 value from 1.3 to 1.5 Gy. In this case, as a result of increased tumor radioresistance, cure is not achieved.
The importance of the model parameters
It is clear from the above scenarios, as well as from clinical experience, that multiple factors likely determine if a course of therapy is curative or not for medulloblastoma. To illustrate the sensitivity of cure, cross-plot analyses of treatment outcome as a function of several tumor and transport parameters was undertaken. In Figure 7, the impact of the values of kg,t, kg,f, γf, γt, D0 and the initial size of the brain tumor (Nb,t) on the maximum duration of treatment break duration is shown.
We have presented a two-compartment kinetic model that describes tumor growth and flow within the closed system of the craniospinal axis. Using model parameters derived from known experimental and clinical data, the simple model was able to generate results that are consistent with clinical observations. By such validation, it can be properly used by clinicians to achieve a 'first-approximation' prediction of various potential scenarios that may arise in the treatment of medulloblastoma.
The model and equations presented herein are a simplification of a complex process. Three major assumptions have been made in the model's creation. First is the assumption that the logarithm of cell survival is proportional to dose, or that the fraction of remaining cells is equal to . This is true for cells in the linear portion of cell survival curves, but not in the shoulder region where fractionated radiotherapy takes place. However, there is a minimal shoulder to medulloblastoma cell survival curves, so this assumption is probably reasonable .
Second, it has been assumed that the cells from the primary tumor are constantly disseminating in the CSF and forming satellite nodules that can then themselves disseminate immediately. This is almost certainly not the case for all tumors, especially those early in their growth .
Third is the fact that assumptions for the values of the rate constants have been made. The process of cell shedding from tumor masses in a circulating fluid, be it CSF or blood, is not well characterized, and the rate constants used in the analysis are extrapolations from limited data. The value of kshed and kadh are probably less than what was used in the analysis, since there are other factors besides cell shedding that make an observed doubling time for a tumor longer than Tpot. It is also well known that not all tumors with access to the CSF circulate through it, or at least not to levels that lead to clinical complications, implying that kshed for these tumors is exceedingly low. For example, CSI was once the treatment of choice for intracranial germinomas [22, 23]. However, more recent studies evaluating whole ventricle-only or whole brain-only treatment show that more limited treatment fields can lead to cure in many patients, indicating that (clinically relevant) spread to the spine is not a foregone conclusion in some diseases [24, 25]. We have used the modulating factors γf and γt to describe the potential impact of changes in the kshed and kadh values on treatment outcome.
The assumption that there is no potential for 'escape' of cells circulating in the CSF to the circulatory system has also been made. This is a reasonable assumption given the exceeding rarity of extracranial metastases . Many extracranial metastases are in fact intraperitoneal in origin, and arise in the setting of shunts that divert CSF into this space.
Finally, the assumption that the CSF contents are homogenous throughout the course of the craniospinal axis has been made. This may not be the case in all circumstances . Incorporation of changes in cell density in the different compartments could be incorporated in future versions of the model. If tumor cell density is higher in the spine than in the brain, spine treatment breaks would likely lead to lower cure rates.
Why one tumor type can spread freely in the CSF and another remains more localized (i.e., why kshed and/or kadh differs between tumors) is not known. Molecular determinants of tumor cell invasiveness, such as cadherin expression, probably play a role. E-cadherin governs cell-cell contact and reduced expression of E-cadherin allows cells to separate from their neighbors and invade locally and distantly. Utsuki et al found E-cadherin was not expressed on any of the medulloblastoma cells studied . Asano et al showed that reduced levels of N-cadherin were seen in astrocytic tumors that had disseminated via the CSF . The values of kshed and kadh may in part be functions of the status of proteins such as the cadherins in tumors.
Although the growth rate constant for tumors used in the analysis is a reasonable value, the growth rate of cells circulating in the cerebrospinal fluid is less well understood. This environment may or may not be conducive to cell growth. Figure 7 shows the modest difference on treatment outcome between allowing versus not allowing tumor cell growth in the fluid phase of the model.
Despite these limitations, the model provides insight into the relationship between tumor growth, CSF flow, and radiation-induced cell killing. Modest changes in rate constant values, tumor growth rates, and/or tumor radiosensitivity will not change the general conclusions that emerge from it. Figure 7 again illustrates the potential impact of changes on certain of the model parameters on treatment outcome.
The cross-plots shown in Figure 7 may have direct clinical value for oncologists. Success or failure of a treatment regimen is quite sensitive to small variations in the starting tumor cell number and radiosensitivity. The most direct method of achieving a smaller initial tumor size is to perform a more complete surgery, though a maximum safe resection frequently dictates that some gross tumor be left behind to minimize morbidity. Alternatively, chemotherapy can reduce the tumor burden when administred before and/or with radiotherapy. In addition, chemotherapy may substantially increase radiosensitivity (i.e., decrease D0).
The parallels between CSF dissemination and hematogenous metastasis are obvious, but one point bears special mention. In our model, completion of the brain treatment initially leads to cure within this space (i.e., no tumor cells left). However, if the spine is left untreated, it will eventually re-seed the brain space and lead to tumor growth there. In this setting, the spine can be thought of as the 'primary' site and the brain as the 'metastatic' site. With the primary site left uncontrolled, the chance of developing metastatic sites is ultimately inevitable in this model. Many in the clinical oncology community have emphasized the importance of local therapies to prevent distant failures . Aggressive attempts at local control can minimize such failures.
Craniospinal irradiation remains an important component of the treatment of medulloblastoma. It is critical that clinicians are aware of the propensity of medulloblastoma cells to disseminate throughout the craniospinal axis. The model presented in this paper uses established medulloblastoma-related parameters to describe this dissemination and predict its complications. It reinforces the importance of good clinical practices, such as minimizing the duration of treatment breaks in the irradiation of the spinal fields, to improve the chance of favorable outcome. The model also suggests that the addition of other therapeutic modalities, such as chemotherapy, can significantly reduce the risk of treatment failure by relatively small improvements in radiosensitvity and/or lower tumor burden.
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This work was presented as a poster at the 88th annual meeting of the American Radium Society. We thank Siddhartha Jain for helpful discussions.
The author(s) declare that they have no competing interests.
JM helped conceive of the model, analyzed the scenarios, and drafted the manuscript. EH and LM provided insights into the model structure and edited the manuscript. JK conceived of the model and helped to draft the manuscript. All authors read and approved the final manuscript.
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