This application is based upon and claims the benefit of priority from European Patent Application No. 02425157.1 filed on Mar. 15, 2002, the entire contents which is expressly incorporated herein by its reference.
The present invention relates to a method for estimating or predicting the anti-tumor activity of a compound and for estimating or predicting the tumor growth in mammals.
The in vivo evaluation of the anti-tumor effect of a drug is a fundamental step in the development and evaluation of anti-tumor drugs. In some experiments, tumor cells from immortalized cell lines are inoculated in animals, for example in nude mice, commonly randomised between control and treated animals; in other experiments, tumors grow spontaneously in animals. When a minimal standardised tumor mass is reached, either the vehicle or the active drug treatment are given to control and treatment animals, respectively. The tumor volume is then measured at different times throughout the experiment. It is known to define the effect of the drug on the tumor growth by calculating the inhibition of the tumor growth compared to that observed in control animals at a defined time after the end of the treatment, or by underlining the increase in survival time, expressed as the increase of time required to achieve a certain tumor mass.
This approach is known for defining the most efficient drug candidate within a series of drugs and/or for testing different dosage regimens.
To describe the dynamics of the tumor growth, a number of mathematical models is known; yet, the equations used are either purely empiric and comprise parameters without a biological meaning, or are so complex that it is impossible to derive reasonable estimates from the experimental data.
The use of empirical mathematical equations (e.g. sigmoidal functions such as logistic, Verhulst, Gomperts, von Bertalanffy) is known in order to describe the growth curve of macroscopic variables such as volume, mass or size of cellular population (e.g., Maru{haeck over (s)}iae, M.; Bajzer, {haeck over (Z)}. Generalized two-parameter equation of growth. J Math Anal Appl 1993, 179, 446-461; Bajzer, {haeck over (Z)}.; Maru{haeck over (s)}iae, M.; Vuk-Pavlociae, S. Conceptual frameworks for mathematical modeling of tumor growth dynamics. Mathl Comput Modelling. 1996, 23, 31-46); their aim is to predict the tumor growth even without an in-depth mechanistic description of the underlying physiological processes, so that they are typically defined using parameters with limited biological relevancy and they have little predictive power.
Most often, the growth of biological systems, from a phenomenological and macroscopic point of view, is described by empirical curves with sigmoidal profile. In the in vivo tumor growth kinetics, the tumor mass is treated as a population of homogeneous cells in which the fluctuations and the demographic structure have negligible effects on the macroscopic dimensions of the tumor. The imposition of a sigmoidal profile to the tumor mass finds its own theoretical base in the general observation that the observed solid tumors slow down their own growth, as soon as they become greater, up to reach an asymptotic value (plateau). Denoting the weight of the tumor with W(t), a possible mathematical paradigm for empirical models is furnished by the following autonomous differential equation with initial value W0:
where G(W(t))>0 represents the effective rate of growth, while D(W(t))>0 represents the degradation one. Both functions are differentiable increasing functions, coinciding in correspondence of the plateau {overscore (W)} and such that G(W0)>D(W0). The various models heretofore applied are described by equations (von Bertalanffy, Logistic Growth, Gompertz equation, etc.) that are particular cases of the (5.1) on the base of different choices of the functions G(W(t)) and D(W(t)) (Bajzer, {haeck over (Z)}.; Maru{haeck over (s)}iae, M.; Vuk-Pavlociae, S. Conceptual frameworks for mathematical modeling of tumor growth dynamics. Mathl Comput Modelling. 1996, 23, 31-46). Despite the similar mathematical structure, only the model described by Gompertz succeeds in adequately describing a large range of experimental data, although the interpretation of its biological meaning still appears difficult (G. G. Steel, “Growth kinetics of tumours”, Clarendon Press, 1977).
Functional models, conversely to the empiric approach, are based on a set of assumptions about biological growth from a mechanistic, physiologically based point of view, involving cell-cycle kinetics and biochemical processes such as those related to angiogenesis and/or immunological events (e.g. Bajzer et al., 1996, ditto; Bellomo, N.; Preziosi, L. Modeling and mathematical problems related to tumor evolution and its interaction with the immune system. Mathl. Comput. Modelling 2000, 32, 413-452). Such models usually represent the cell population in its heterogeneity; in the simplest case, the whole population consists of two subpopulations only: the proliferating and the quiescent one. More complex models describe the cell population as age structured and take into account more than two subpopulations related to specific phases of the mitotic cell cycle. Functional models, based on biological principles, are generally complex and have a greater number of parameters compared to empirical models. As a consequence, they are not that useful in an industrial context. Their development is time-consuming and a number of mechanistic observations (e.g., flow cytometry analyses, biochemical, immunological markers measurements etc.) are required to avoid the identifiability problems due to the “overparametrization”.
The situation becomes even more complex when the effect of the treatment with an anticancer drug needs to be considered (R. K. Sachs, L. R. Hlatky and P. Hahnfeldt, “Simple ODE Models of Tumor Growth and Anti-Angiogenic or Radiation Treatment”. Mathematical and Computer Modelling, 33: 1297-1305, 2001; A. Iliadis and D. Barbolosi, “Optimizing Drug Regimens in Cancer Chemotherapy by an Efficacy-Toxicity Mathematical Model”. Computers and Biomedical Research, 33: 211-226, 2001, D. Miklavèiè, T. Jarm, R. Karba and G. Ser{haeck over (s)}a, “Mathematical modeling of tumor growth in mice following electrotherapy and bleomycin treatment”. Mathematics and Computers in Simulation, 39: 597-602, 1995; Panetta J. C. A mathematical model of breast and ovarian cancer treated with paclitaxel. Mathl Biosci 1997, 146, 89-113) due to the uncertainties regarding the mode of action.
A first attempt for simplifying the problem was proposed by Dagnino G, Rocchetti M, Urso R, Guaitani A, Bato{haeck over (s)}ek I. Mathematical modeling of growth kinetics of Walker 256 carcinoma in rats. Oncology 1983, 40, 143-147, (referred hereinafter as Tumor Perfusion Model), the growth of a population of tumor cells is limited by the availability of nourishment perfused to the neoplastic tissue by the systemic circulation. The fundamental hypothesis is that the perfusion capability, then the delivery of nutrients, decreases with the expansion of the neoplastic tissue and, consequently, the reduction of the growth rate of the tumor mass. The phase of growth is thus subdivided in three phases:
Starting from the subdivision of tumor cells in two populations (the proliferating and the quiescent ones) and denoting the respective masses with L(t) and with M(t), the model determines an expression for the total weight W(t) of the tumor in each of the three phases of growth. Consider the following system of differential equations:
with initial conditions L(0)=L0 and M(0)=0, in which the functions λ(t) and μ(t) represent respectively the reproduction rate of new cells and the rate of passage from proliferation to quiescence.
For each of the three phases it results:
Referring to Dagnino et al. (ditto) for the calculations, an analytical expression for the macroscopic weight of the tumor W(t)=L(t)+M(t) in the three phases is provided:
W(t)=L0·exp(λ0 0≦t≦t1 (5.4)
W(t)=L0·exp(λ0·t1)+λ1·(t−t1≦t≦t2 (5.5)
satisfying the conditions λ0·W(t1)=λ2 and λ0·W(t2)=λ1 in order to ensure W(t)εC1.
Although this model was efficient enough for describing the tumor growth, the equations therein used (5.4 and 5.6) describe only the tumor growth broken in the different steps and it did not include the effect of a possible treatment.
A method which makes the best use of all the information generated during the preclinical studies and applicable in the pharmaceutical field is still missing.
An object of the invention is therefore to provide a method for estimating or predicting the anti-tumor activity of a compound administered to mammals developing a tumor as well as a method for estimating or predicting the tumor growth in said mammals which result to be sufficiently simple and allow to get good estimates or predictions regardless of the uncertainties on the mode of action.
Among the objects of the invention, there is that of employing a small number of parameters so to be useful in an industrial context and therefore avoiding time consumption as well as a number of mechanistic observations.
A further object of the invention is that of estimating or predicting different schedules of the tested compound, therefore permitting a better understanding of the mechanism of action of the compound as well as to optimise the experimental designs and results.
Still further, an object of the invention is that of providing a method which may increase the throughput of tumor growth inhibition experiments, permits less schedules to be tested and a lower number of mammals and lower amounts of the tested compound to be used for evaluating the efficacy of the compound, and permits a classification and a comparison of tested compounds.
These and other objects, which will be apparent from the understanding of the following description, are attained by the methods of the invention; in particular, according to a first aspect of the invention, by carrying out a method for estimating the anti-tumor activity of a compound administered to mammals developing a tumor comprising:
A further parameter (ψ), representative of the tumor growth curves shape, is preferably calculated; in particular, L0, λo, λ1, K1 and K2 are calculated using a non-linear fitting program, which finds the best combination of the parameters, comparing -in time- the measured tumor weights with the tumor weights calculated by the program, by the following system of ordinary differential equations and initial conditions:
wherein
Preferably, the method for estimating the anti-tumor activity comprises evaluating the survival time (τ) of damaged tumor cells in transit inside the chain of mortality, described through a random variable τ for which a probability density function pdf(τ) is considered; said pdf(τ) being described, by applying a compartmental model comprising n-1 compartments, as above defined, with first-order kinetics, regulated by K1 and Zi(t) as above defined; said compartmental model being described by the following system of differential equations:
{dot over (Z)}2(t)=K2·c(t)·Z1(t)−K1·Z2(t)
{dot over (Z)}3(t)=K1·Z2(t)−K1·Z3(t) (6.2)
{dot over (Z)}i(t)=K1·Zi-1(t)−K1·Zn(t)
wherein Zi(t), i, t, n, K1 and K2 are as above defined; under the hypothesis that the tumor mass in exit in the time unit from a compartment is proportional to the resident mass according to K1 and considering that the growth of Z1(t) is
{dot over (Z)}1(t)=f(W(t))−K2·c)(t)·Z1(t) (6.1)
wherein f(W(t)) represents the equation of the tumor growth of the mammals to which the compound has not been administered, function of the tumor total weight W(t).
The probability density function pdf(τ) has generally a bell-like shape and is an Erlang(n-1, K1):
wherein K1, t and n are as above defined;
Ψ is preferably fixed to 20 while the best combination of the above kinetic and pharmacodynamic parameters may be carried out by the technique of the weighed least squares; the tumor measurement error may be determined by the following measurement error model:
DMIN=D{circumflex over ( )}MIN+εMIN (3.3)
DMAX=D{circumflex over ( )}MAX+εMAX (3.4)
Preferably, the calculation of the tumor growth curves comprises a delay of time (tlag) between the moment in which the tumor mass is damaged by the aggression of the compound and the instant in which the mass enters the chain of mortality; in particular this can be realised inserting a delay in the time of administration of the compound to the mammals.
To estimate the anti-tumor activity of the compound, the kinetic parameters K1 and K2 may be either directly measured or derived from known estimates of the same tumor cell line on the same mammals obtained by previous experiments.
A second aspect of the invention concerns a method for predicting the anti-tumor activity of a compound administered to mammals developing a tumor, comprising:
Preferably, the method for method for predicting the anti-tumor activity of a compound according to the invention comprises evaluating the survival time (τ) of damaged tumor cells in transit inside the chain of mortality, described through a random variable τ for which a probability density function pdf(τ) is considered; said pdf(τ) being described, by applying a compartmental model comprising n-1 compartments, as above defined, with first-order kinetics, regulated by K1 and Zi(t) as above defined; said compartmental model being described by the following system of differential equations:
{dot over (Z)}2(t)=K2·c(t)·Z1(t)−K1·Z2(t)
{dot over (Z)}3(t)=K1·Z2(t)−K1·Z3(t) (6.2)
{dot over (Z)}i(t)=K1·Zi-1(t)−K1·Zn(t)
wherein Zi(t), i, t, n, K1 and K2 are as above defined; under the hypothesis that the tumor mass in exit in the time unit from a compartment is proportional to the resident mass according to K1 and considering that the growth of Z1(t) is
{dot over (Z)}1(t)=f(W(t)−K2·c(t)·Z1(t) (6.1)
wherein f(W(t)) represents the equation of the tumor growth of the mammals to which the compound has not been administered, function of the tumor total weight W(t).
The probability density function pdf(,) has preferably a bell-like shape and is an Erlang (n-1, K1):
wherein K1, t and n are as above defined;
The tumor growth curves may be calculated using a program which predicts the tumor weight by the following system of ordinary differential equations and initial conditions:
{dot over (Z)}2(t)=K219 c(t)·Z1(t)−K1·Z2(t) Z2(0)=0 (6.9)
{dot over (Z)}3(t)=K1·Z2(t)−K1·Z3(t) Z3(0)=0 (6.10)
{dot over (Z)}4(t)=K1·Z3(t)−K1·Z4(t) Z4(0)=0 (6.11′)
wherein:
The compound tested according to the invention is preferably an antitumor agent. In particular, the compound is paclitaxel or brostallicin.
The concentration of the compound is either directly measured or indirectly determined from pharmacokinetics models of interspecies scaling i.e. extrapolating the concentration of the compound from known experimental data on different species (see, f.i. Dedrick R L. Animal scale-up, Journal of Pharmacokinetics & Biopharmaceutics. 1(5):435-61, 1973 October UI: 4787619; Boxenbaum H., “Time concepts in physics, biology, and pharmacokinetics”, Journal of Pharmaceutical Sciences. 75(11):1053-62, 1986 November; Mordenti J. “Man versus beast: pharmacokinetic scaling in mammals”, Journal of Pharmaceutical Sciences. 75(11):1028-40, 1986 November) The concentration of the tested compound is preferably measured in plasma, serum or tissue.
The above methods, according to the first and second aspects of the invention, can also be advantageously carried out for evaluating the mechanism of action of a compound administered to mammals developing a tumor. In particular, the tumor growth curves can be calculated using a program which predicts the tumor weight by the following system of ordinary differential equations and initial conditions:
wherein γi is an index, possibly equal to zero, of the rate of tumor cells in the i-th compartment that recover from their damage, while L0, λo, λ1, K1, K2, Ψ, Z1(t), Zi(t), i, n, t and c(t) are as above defined; the calculated tumor weight W(t) being
wherein Zi(t), i, n and t are as above defined.
Further, the above methods, according to the first and second aspects of the invention, can also be advantageously carried out for estimating a minimal steady state compound concentration to be maintained for observing tumor regression in in vivo experiments. In fact, it comes out, from (6.8-6.11), that under a constant compound concentration, the zero state, corresponding to a tumor weight equal to zero is a stable equilibrium if the concentration is greater than λ0/K2 (which corresponds to the minimal steady state concentration of the compound).
Still further, the above methods, according to the first and second aspects of the invention, can also be advantageously carried out for testing the additivity of the effect of at least two compounds on the tumor growth in in vivo experiments; in particular, the tumor growth curves are calculated using a program which predicts the tumor weight by the following system of ordinary differential equations and initial conditions:
wherein:
Still further, the invention concerns the use of the calculation of the tumor growth curves according to any of the above aspects of the invention, for predicting the optimal administration dosage/schedule of a compound for the preparation of a medicament for the treatment of tumor.
A third aspect of the invention concerns a method for estimating the tumor growth in mammals developing a tumor, comprising:
The parameter A, as above defined, is also preferably calculated or, more preferably, it can be fixed to 20. The tumor growth may be calculated by a statistical program and defined by the following function:
wherein:
The tumor measurement error can be determined by the measurement error model above illustrated for the method for estimating the anti-tumor activity.
A fourth aspect of the invention concerns a method for predicting the tumor growth in mammals developing a tumor, comprising:
ψ is preferably fixed to 20 whereas the tumor growth may be calculated by a statistical program and defined by the following function:
wherein:
The non-linear fitting or statistical program for any of the methods of the invention is preferably WinNonLin® 3.1.
The above illustrated methods of the invention preferably comprise a statistical program simultaneously fitting tumor growth curves of individual values or of the mean values for implementing any of the above methods; in particular, the statistical program is NONMEM, a software for population pharmacokinetic analysis which can be supplied by the NONMEM Project Group C255 University of California at San Francisco, San Francisco, Calif. 94143.
Any of the methods of the invention are preferably carried out by subcutaneously inoculating the mammals, in particular nude mice, with tumor cells so to develop a tumor. The parameter L0 would therefore be, according to this preferred embodiment of the invention, representative of the portion of the inoculated tumor cells that succeeds in taking root and in starting the tumor cells proliferation in subcutaneous tissues of the mammals.
A further aspect of the invention also concerns a computer program for estimating or predicting the anti-tumor activity of a compound administered to mammals developing a tumor, or for estimating or predicting the tumor growth in said mammals comprising computer code means for implementing any of the above illustrated aspects of the invention.
The term “mammals” is herein meant to refer to animals only whereas either the term “compound” or “drug” are herein meant to comprise any molecule tested either for estimating or predicting the possible anti-tumor activity thereof.
According to a preferred embodiment of the invention, two different experiments were made in order to test the invention. These experiments are described in detail below. With these experiments some studies of efficacy of two supposedly anti-tumor drugs: drug-A and drug-C have been conducted regarding the in vivo growth of human tumor cell lines, inoculated in athymic nude mice.
Drug A is paclitaxel. Drug C is brostallicin; the compound is characterised in WO98/04524 and can be prepared as therein disclosed.
The two experiments involve the use of two populations of subjects: the controls and those subjects that receive the pharmacological treatment. The term “control” is preferred in the present specification to the term “not treated”: in fact, in order to eliminate the variables which invalidate the results, even on the mice that do not receive the drug, the administration of active excipients (vehicle or placebo) is practiced, as a rule, adopted together with the drug in order to improve its solubility and its ability of distribution in the tissues (Paroli E., “Farmacologia di base, preclinica, clinica”, Farmacologia clinica tossicologica, Soc. Editrice Universo, Roma, 1985; A. Henningsson, M. O. Karlsson, L. Viganò, L. Gianni, J. Verweij and A. Sparreboom, “Mechanism-Based Pharmacokinetic Model for Paclitaxel”, Journal of Clinical Oncology, 19 (n. 20-October 15): pp. 4065-4073, 2001). In all experiments, the tumor was inoculated into the animals in a subcutaneous position (on the back). The day of the inoculum was assumed as the origin of the time scale of the experiment and subsequently referred as day-0. The animals were divided in the different cages, maintained under sterile environmental conditions with controlled temperature and light (12 h/day), with free access to food and water (ad libitum). The pharmacological treatment (as the one with vehicle only for the controls) started at the end of the so-called “silent interval”(G. G. Steel, 1977, ditto). Such expression is often used for denoting the early phase of the tumor growth after the inoculum, wherein the tumor cells, even if present and proliferating, have not yet produced a detectable and measurable tumor mass. The first measurement of the tumor mass was executed as the treatment began.
The mice were then withdrawn from the cages and weighed, executing the measurements for the determination of the tumor mass as described in the experiments hereinafter; for some of them, plasmatic samples were drawn in order to determine the concentration of the selected drug.
At the end of the period of observation the animals were sacrificed for autoptic inspections.
The invention will be more apparent from the accompanying drawings, which are provided by way of non limiting example and wherein:
Experiment-A
The cell line GTL16 (human stomach carcinoma) was inoculated subcutaneously on the back of 44 athymic nude male mice, initially weighing 17.9-28.1 g. The animals were then subdivided in four cages:
The treatment and the first measurement of the tumor mass took place on the eighth day after the inoculation. For each of the cages G2, G3 and G4, four mice were withdrawn for monitoring the plasma concentration of the drug. The experiment had a total duration of 40 days.
The following Tab.1 provides a summarizing scheme of the protocol adopted for the Experiment-A.
Experiment-C
The cell line H207 (ovarian human carcinoma) was inoculated subcutaneously on the back of 70 female athymic nude mice, initially weighing 17.0-25.0 g. The animals were then subdivided in ten cages:
In this case, despite the silent interval finished in correspondence of the tenth day (where the first measurement of the tumor mass was carried out), the chemotherapeutic treatment started in correspondence of the eleventh day. The experiment had a total duration of 89 days.
The following Tab. 3 provides a summarizing scheme of the protocol adopted for the Experiment-C.
Approximation of the tumor Mass
The dimensions of the tumor can be taken applying different types of measurements broadly classifiable as measurements of linear dimensions, of volume (or mass) and cell number. For tumors that maintain more or less a spherical morphology, as in the case of solid tumors, the measurement of the three principal diameters results the most adequate, as well as the most practiced solution. Nevertheless, in the case of subcutaneous tumors, the tumor can be considered of spherical shape only during the initial phase of growth; in the following phases, the dimension perpendicular to the skin is generally much smaller than the percutaneous dimensions, conferring to the mass a plaque-like shape or an hemi-ellipsoidal shape. In the experiments taken into consideration, only the dimensions of the two percutaneous diameters were directly measured with vernier calipers. The third dimension was not directly measured, because of the limited accessibility (which would have required a greater invasiveness), in the assumption that two measures were anyhow sufficient to guarantee a good approximation of the tumor mass (K. Rygaard and M. Spang-Thomsen, “Quantitation and Gompertzian analysis of tumor growth”. Breast Cancer Research and Treatment, 46: 303-312,1997).
The volume of a tumor can be indirectly calculated by applying the following empirical formula:
where DMIN and DMAX denote, respectively, the smallest and the largest percutaneous diameter. Such empirical formula hypothesizes that the neoplasia has an ellipsoidal shape (D. A. Cameron, W. M. Gregory, A. Bowman, E. D. C. Anderson, P. Levack, P. Forouhi and R. F. C. Leonard, “Identification of long-term survivors in primary breast cancer by dynamic modeling of tumour response”. British Journal of Cancer, 83(1): 98-103, 2000, Hammond, L. A.; Hilsenbeck, S. G.; Eckhardt, S. G.; Marty, J; Mangold, G.; MacDonald, G. R.; Rowinsky, E. K.; Von Hoff, D. D; Weitman S. Enhanced antitumour activity of 6-hydroxymethylacylfulvene in combination with topotecan or paclitaxel in the MV522 lung carcinoma xenograft model. European Journal of Cancer 2000, 36, 2430-2436) obtained by the rotation of a hemi-ellipsoid (with DMIN and DMAX as axes of the percutaneous plane) around its largest axe. Assuming δ as a constant density equal to δ=10−3g/mm3, the empirical expression for the mass of the neoplasia results to be:
The Measurement Error Model
The measurement of the diameter of a tumor, on animals of laboratory, is not always an easy task even with the use of anaesthetics. In fact experimental tumors show a high variable firmness; as a consequence, in the case of the more flabby tumors, the entity of the measurement depends in a significant manner on the pressure which is applied to the caliper. A further complication is represented by the skin thickness which risks to spoil the measurement. In all these cases it is advisable either to indicate an average value of the measurements made by several observers or to employ a single observer throughout all the measurements of the experiment.
Despite the due precautions, the measurements of the two percutaneous diameters are to be considered not devoid of errors. In particular, the presence of an error which is of additive type and proportional to the real value of the diameter, according to the constant CV (coefficient of variation) is herein assumed. The effective measurements (DMIN and DMAX) are therefore bound to the real values of the two diameters (DMIN and DMAX) through the following relationships:
DMIN=D{circumflex over ( )}MIN+εMIN (3.3)
DMAX=D{circumflex over ( )}MAX+εMAX (3.4)
where εMIN and εMAX represent the measurement errors, for which it is assumed:
Var[εMIN]=CV2·D2MIN (3.5)
Var[εMAX]=CV2·D2MAX (3.6)
{circumflex over ( )}
Denoting the tumor weight with W and considering (3.2), it is then possible to obtain an expression for the tumor weight variance, Var[W]: {circumflex over ( )}
Substituting (3.5) and (3.6) into (3.7), with a further approximation DMIN≅DMAX, after some simple passages, it can be obtained:
Var[{circumflex over ( )}]≅ξ2·W2 (3.8)
wherein Ŵ is the experimental value of W and ξ is a proportionality factor to CV.
The expression (3.8) allows to determine the optimal weighing strategy of the observed data, which can be used in the algorithm of non linear regression, by which the fitting is computed.
The Fitting
The software used for the fitting of the various models (both the PK model and the ones descriptive of the tumor growth) uses an algorithm of non linear regression based on the Least Squares and a Gauss-Newton algorithm with Levenberg-Hartley modification (H. O. Hartley, “The modified Gauss-Newton Method for the Fitting of Nonlinear Regression Functions by Least Squares”. Technometrics 3, 1961). Since the error model related to the various experimental measurements is unknown for fitting pharmacokinetic models, a standard least squares technique (Least Squares, LS) has been used according to what disclosed in J. V. Beck and K. J. Arnold, “Parameter Estimation in Engineering and Science”. John Wiley & sons, 1977, herein incorporated as a reference as far as the least square technique is concerned.
As it regards the model of tumor growth, the error model above introduced is instead known. For the observed measurements of a generic quantity y (for instance the weight of the tumor), the constant coefficient of variation error model (3.5 and 3.6) asserts that the standard deviation of the error varies linearly with the dimension the measured quantity. With an error model of this kind, the technique of the weighed least squares (Weighed Least Squares, WLS), described in M. E. Dagna, “Identificazione di modelli farmacocinetici di popolazione”; Università degli Studi di Pavia 1999, herein incorporated as far as the WLS technique is concerned, is more adequate. The WLS criterion determines the vector θ, of the parameters to be identified, so to minimize an objective function with the following structure
where y{circumflex over ( )}j denotes the j-th predicted value of the variable y (in correspondence of the observed value yj, while the term wj is the weight related to the j-th observation, proportional to the inverse of the variance of the j-th measurement error (defined by the 3.8). Such a weighing strategy, gives less importance to the residuals related to big values of the quantity y, taking into more account the residuals related to small values of the same quantity y. The standard LS technique is then a particular case of the WLS technique wherein a uniform weighing strategy is adopted.
The Experimental Data
The experimental observation, related to the two experiments described before, are graphically represented in
For the Experiment-A, the following data are available:
For the Experiment-C, the average measurements of the tumor weight are available (
The Pharmacokinetic (PK) and Pharmacodynamic (PD) Approach
The most common approach to the in vivo pharmacokinetic and pharmacodynamic model identification involves the sequential analysis of the concentration of the tested compound versus time and therefore the study of the time course of the effect. The PK model, obtained in the first step, provides an independent function able to drive the dynamics (
The understanding of the basic concepts regarding the absorption of a drug, the distribution, metabolism and elimination (ADME), thereof as well as the relationship between kinetics and dynamics, is a fundamental aspect of the PK/PD modeling. Despite the purpose of this invention is beyond the treatment in detail of the pharmacokinetic theory, it is deemed to be opportune to introduce some fundamental concepts hereinafter applied.
Pharmacokinetics and Pharmacodynamics
Pharmacokinetics is the study of the rate and mechanism through which a drug is absorbed in the organism, distributes itself into it and is eliminated from it through metabolic and excretion processes. In less rigorous terms, pharmacokinetics is often defined as “what the body does to a drug and at which rate”, in opposition to pharmacodynamics, which studies “what the drug does to the body”. Strictly speaking, pharmacodynamics can be defined as the study of the biochemical and physiological effects of a drug and of its mechanism of action. Such discipline determines therefore, the relationship among the pharmacology response (effect) and the concentration of the drug or of some of its metabolites.
Pharmacokinetics is tipically studied measuring the time course of the drug concentration in plasma although, as above stated, in the present invention, the drug concentration can also be measured in serum or tissue. The profiles of the concentrations of the tested compound versus time can be described in empirical way (non-compartmental pharmacokinetics), defining the entities of the measured concentrations, the slopes (correlated to the rates of the processes) and the integral of the curve (AUC, Area Under the Curve). From a more modelistic point of view, the compartmental pharmacokinetics can be exploited; the organism, according to this approach, can be assimilated to a system of one or more compartments where the drug enters, distributes, degrades and is excreted. This does not mean that the compartment corresponds to a specific anatomical entity or to a real physiological one, but that it can be assimilated to a tissue or to a set of tissues which possess some affinities for the drug, within which the drug moves and goes out with a rate of change proportional to its concentration (first-order kinetics). In the models based on the compartmental analysis the tendency is to always employ the least number of compartments necessary to adequately describe the experimental results. In a multi-compartment model the drug is quickly distributed in those tissues that have high hematic flows: the blood and these highly perfused tissues constitute the central compartment. While this initial diffusion of the drug is taking place, it is also distributed in one or more peripheral compartments constituted by the less perfused tissues, having similar hematic flows and affinity for the drug. In this case, a multi stage exponential decay will be observed on the profile of the concentration of the tested compound versus time curve. Remembering the hypothesis which assumes a first-order kinetics associated to each compartment, a number of compartments equal to the number of exponential stages will be then employed. Compartmental pharmacokinetics is illustrated, for instance, in J. G. Wagner, “Biopharmaceutics and relevant Pharmacokinetics”. Drug Intell, Publ. Hamilton, 1971, M. Gibaldi and D. Perrier, “Pharmacokinetics”. Marcel Dekker, 2nd Ed., New York, 1982, L. Shargel and A. B. C. Yu, “Biofarmaceutica Farmacocinetica”. Masson Italia Editori, Milano, 1984, M. Rowland and T. N. Tozer, “Clinical Pharmacokinetics: Concepts and Applications“. Lea & Fabinger, 2nd Ed., 1989, J. Gabrielsson and D. Weiner, “Pharmacokinetic/Pharmacodynamic Data Analysis: Concept and Applications 2nd Ed.”, Apotekar Societen, 1997 herein incorporated as a reference as far as this issue is concerned.
Experiment-A: PK model and fitting
From the observation of the experimental curve of the plasma concentration of Drug-A (
The constant K10 (expressed in day−1) represents the constant rate of the elimination process (hypothesized only in the central compartment). K12 and K21 (expressed in day−1) represent the interchange constant rates between the central compartment and the peripheral one. VD is the so called apparent volume of distribution of the central compartment; it is expressed in ml kg−1 and represents the hypothetical volume in which the drug dose would distribute if the distribution process was uniform.
“Pharmaceutical treatment” is herein meant to generically indicate whichever kind and route of administration of at least one selected compound; in the present experiment, an intravenous bolus of the drug dose D in input was administered at the time t0. The absence of the absorption compartment allows to model the bolus, from the point of view of the central compartment, as a Dirac delta function centered around t0 having an area equal to the administered dose D. According to the adopted bi-compartmental model, the concentration of the tested drug in the central compartment, in response to the single bolus, can be expressed by the following equation:
c(t)={A·exp[−α·(t−t0)]+B·exp[−β(t−t0)]}·H(t−t0) (4.1)
in which H(·) is the Heaviside unitary step function, while A, B, α and β are the four macro constants (characteristic parameters of the model), in contrast to K10, K12, K21, and Vc (volume of distribution of the central compartment) called micro constants. Both types of constants can be univocally derived from one another and vice versa (as disclosed, f.i., in M. Gibaldi et al., 1982, ditto, herein incorporated as a reference as far as this issue is concerned).
The therapeutic regimen of the Experiment-A adopts the administration of three repeated intravenous boluses at the distance of four days each; the input function of central compartment is therefore expressible as:
wherein DG and ti represent the dose associated to each cage and the instants of administration (t1=8, t2=12, t3=16) respectively. Exploiting the linearity of the compartmental models and the expression of the concentration in response to a single bolus is possible to analytically define the course of the concentration of the tested compound in response to the treatment specified by the (4.2):
The bi-compartmental model has been therefore tested against the experimental data. It was decided to estimate the four macro-constants because from the observation of the profile of the observed data it has been possible to furnish an initial adequate estimation thereof; subsequently, an indirect estimation of the four micro-constants has been determined. The results of the fitting are shown in Tab. 4.1 and in Tab. 4.2.
Descriptive statistics (mean, standard deviation and coefficient of variation) of macro and micro constants are presented in tables 4.3 and 4.4.
The two-compartment PK model, employed for describing the pharmacokinetics of the Drug-A, allowed to get satisfactory individual results (the estimation of the four macro-constants). Only for three mice (No. 59, 78 and 81) the predicted profile of concentration seems to have an anomalous time course; in particular, a very slow phase of decay is observed (an excessively low value for the estimation of the macro-constant β). It seems obvious to suppose that such phenomenon is mainly imputable to the lack of experimental data in correspondence of the phase of elimination (related to the parameters B and β).
Considering the parameters values, a great inter-individual variability is however denoted, mainly regarding exactly the parameters B and β. In order to obtain qualitatively better estimations for such parameters, a more complete sampling scheme between the administration of an intravenous bolus and the following one, would be necessary; this is in contrast with the limitations of the physical endurance of the mice submitted to the monitoring of the plasma concentration.
Regardless of the fact that only five experimental observations were available for each mouse, rather stable individual estimations were obtained (moderately limited CV %) for all the four micro-constants, as well as a reconstruction of the concentration profile which is rather faithful to the experimental data. As a consequence, the observed inter-individual variability was rather limited for all the four micro constants.
Experiment-C: PK Model
The pharmacokinetics of the Drug-C is known and can be described by a three-compartment PK model, whose characteristic micro-constants are known. The three-compartment model is an extension of the bi-compartmental model by the addition of a deep tissue compartment (
A drug which requires a three-compartment model is distributed more quickly in the central compartment, less quickly in a second peripheral tissue compartment and very slowly in a third compartment, that of the deep tissues (little perfused tissues as the bones and the adipose tissues).
The average values for the six micro-constants which define the system are shown in Tab. 4.6.
Model for the Growth of the Controls
According to the present invention, the model for the growth of the controls starts from the model and equations proposed by Dagnino et al. (ditto).
Dagnino's Tumor Perfusion Model rewritten in a differential form results:
In order to ensure W(t)εC1, like in the previous model, the following relationship holds:
λ0·W(t1)=λ1 (5.9)
A first modification to be brought to the model concerns the threshold of the passage between the phase of exponential growth and the phase of linear growth, determined by t1. The localization of a threshold on the time scale appears inadequate for two reasons: the possible arbitrariness in the choice of the initial instant of observation and the impossibility to adequately describe the growth of the tumor if weight oscillations manifested around the value W(t1).
The choice to locate a threshold related to the weight of the tumor derives from the previously described drawbacks. Such value, denoted as W*, may be easily localized in
The model in differential form can then be rewritten in the following manner:
For the sake of brevity the mathematical symbolism {dot over (W)} will be later adopted to denote the first derivative of the tumor weight.
Equations (5.11) and (5.12) define a function {dot over (W)}=f(W(t))∉C1 and moreover the existence of a threshold, in which the growth roughly changes from an exponential profile to a linear profile, which seems poorly realistic for a physiological system; the following step consists therefore in the search of a new function f(W(t))εC1, expressible through a unique analytical expression. The adopted solution is the following:
The equation describes an exponential growth in the first phases (for small W(t)) and a linear growth for high values of W(t). The term at the denominator may be interpreted as a penalty factor of the exponential growth; from a physiological point of view then it may be conceived as an index of the incapability to develop a suitable vascular network through the mechanism of angiogenesis. In the initial phase of growth (small W(t)) the denominator can be approximated to the unity (maximum ability of induction of the angiogenesis), while as soon as W(t) increases, the denominator grows up to approximate the value W(t)·λ0/λ1 in correspondence of which the maximum incapability of perfusion is observed, with consequent degradation to a linear growth of the tumor mass.
Parameters of the Model
The model for the growth of the controls described by the equation (5.13) defines a family of function in the class C1, parametric with respect to the choice of the parameter Ψ, of more squared shape (hence similar to that described by the Tumor Perfusion Model in differential form) with the increasing of such parameter (for this purpose, see
I. L0: it represents the portion of the tumor cells present at the instant t0=0 that succeeds in taking root and in starting the tumor cells proliferation in the mammals. A great inter-individual variability is expected with respect to its value; this is due both to the lack of weight experimental data during the silent period and to the variability in relationship with the survival of the tumor cells during the inoculum. Dimensionally it represents a weight and therefore it is expressed in [weight].
II. λ0: it represents an index of the production rate of the tumor cells during an exponential phase of the tumor growth; in other words, it is the rate of production of new tumor cells and therefore an index of the speed of completion of the cell cycle. An estimation with a low inter-individual variability is expected since its value is related to the particular cell line. Dimensionally it represents the inverse of a time and therefore it is expressed in [time−1].
III. λ1: it represents an index of the tumor cells mass produced in the time unit during a linear phase of the tumor growth; unlike λ0, an obvious inter-individual variability is expected from its estimation since it is related to the capability of the single treated subject to develop a vascular network sufficient for the perfusion of the tumor. Dimensionally expressed in [weighttime−1].
IV. Ψ: it represents an adimensional “shape” parameter of the curve described by the model in differential form. Its value will not be estimated both in order to avoid making difficulties in the fitting procedure from a numerical point of view, and because the profile of the function {dot over (W)}, if sufficiently squared, does not affect the quality of the fitting. A somehow arbitrary value will be then fixed, Ψ=20 (
Experiment-A: Fitting of the Controls
Results of the individual fitting for each of the eight mice belonging to the control group are shown in Tab. 5.1.
Descriptive statistics (mean, standard deviation and coefficient of variation) of the three parameters are shown in Tab. 5.2.
Experiment-C: Fitting of the Controls
The results of the fitting performed on mean value of tumor weight, of the mice belonging to the cage G1, are shown in Tab. 5.5.
The model proposed for describing the unperturbed growth of the tumor provided encouraging results in terms of fitting; despite the limited number of available experimental observations for all the subjects, the individual estimations allow to describe the experimental curve of growth in adequate way. The estimations of the parameters are also rather stable (rather limited CV %) with the only exception represented by the mouse number 86 of the experiment-A. Moreover, the expectations of the difficulty in the estimation of the parameter L0 were respected: in almost the totality of cases, L0 was the parameter with the highest values of CV %, besides stressing the greatest inter-individual variability (see the CVs in the population estimations). The experimental data were not indeed available before about a week from the inoculum of the tumor line and furthermore the behavior of the tumor during the silent period is anything but known (even at macroscopic level). The difficulties in the estimation of such parameter can be explained because the model hypothesizes an exponential growth for such period, that is extrapolated backward, from the first available measurements, during the phase of fitting.
Also the expectations of the inter-individual variability in the estimation of the parameters λ0 and λ1 were respected. While the former is the most stable parameter, with the smallest range of estimated values, since it is in relation with the characteristic inoculated cell line, the latter shows an evident inter-individual variability because it is mainly related to a subjective process (the angiogenesis) and therefore to the capability of each subject to extend, the phase of exponential growth rather than to make it degrade to a linear phase of growth.
Model for the Growth of Treated Subjects: Hypotheses
Before inspecting the various steps of synthesis of the model, it is necessary to introduce some simplifying hypotheses:
As in the case of the model for the unperturbed growth of the tumor, the heterogeneities of the population, from the spatial point of view (position inside the tumor spheroid), and of the age (phases of the cell cycle), will not be considered with the consequent assumption that both the nutrients and the drug are able to reach all the neoplastic cells in the same manner.
Pharmacodynamic Effect
The therapeutic activity of antitumor drugs can be exerted in different ways, but all have the same principal purpose: the reduction (the elimination in some cases) of the cell pathogenous population. This purpose can be achieved either reducing the rate of growth of the population or increasing that of mortality. Independently from the nature of the drug (cytotoxic or cytostatic agent), the drug detectable effect, caused by the mechanism of action thereof is the reduction of the effective rate of growth. It is herein assumed that the chemotherapeutic treatment acts by increasing the mortality of the tumor cells (a typical mechanism of action of cytotoxic agents), modeling a perturbation to the unperturbed tumor growth kinetics through the introduction of a term of loss in the equation (5.13). The action of the chemotherapeutic agent leads to the introduction in the (5.13) of a negative term, proportional both to Z1(t), defined as the tumor mass “damageable” by the drug action, and to the concentration of the tested compound c(t) through the constant K2. The equation which regulates the growth of Z1(t) can be then rewritten in the following way:
{dot over (Z)}1(t)=f(W(t))−K2·c(t)·Z1(t) (6.1)
wherein f(W(t)) represents the equation of the growth of the controls, function of the total weight W(t).
For better understanding the pharmacodynamic effect, a functional scheme was used adopting a symbolism similar to that used for the compartmental pharmacokinetic (
The action of the drug is irreversible: the tumor mass, damaged by the chemotherapeutic treatment is no more able to proliferate, leaves the reproducing compartment and, after a certain time delay will die.
Chain of Mortality
The model described by the expression (6.1) involves however that the loss of weight, following the action of the drug, occurs instantaneously. On the contrary, it seems logic thinking that between the instant in which a certain cell is hit and damaged by the drug and the instant in which the cell turns out to be dissolved from the original tumor mass, a finite period of time elapses, necessary to the completion of the mechanism of action and to the decomposition of the damaged mass (because of macrophagous organisms, for instance). In order to avoid any ambiguity it has to be considered that the term “death” refers herein to the instant in which the cell will not furnish its own contribution anymore in terms of weight to the whole tumor mass.
In the developed model, it is hypothesized that the damaged tumor mass enters a “chain of mortality” from which it will exit only when death occurs; up to such event, the mass inside the chain provides a contribution to the total weight of the tumor. The permanence in this chain can be interpreted as the succeeding of stages of progressive degradation, consequent to the aggression of the drug (
The required pdf(τ) may be achieved through the application of the following compartmental approach: consider n-1 compartments with first-order kinetics, regulated by the elimination constant rate K1 (i.e. an index of the tumor cells death rate) and with state variable Zi (i=2, . . . , n-1). The output of the generic compartment Zi constitutes the input for the following compartment Zi+1, with reference to
It is possible for the described compartimental model to write the following differential equations, under the hypothesis that the mass in exit in the unity of time from a generic compartment is proportional to the resident mass according to the elimination constant rate K1 (first-order kinetics):
{dot over (Z)}2(t)=K2·c(t)·Z1(t)−K1·Z2(t)
{dot over (Z)}3(t)=K1·Z2(t)−K1·Z3(t) (6.2)
{dot over (Z)}i(t)=K1·Zi-1(t)−K1·Zn(t)
wherein Zi(t), i, t, n, K1 and K2 are as above defined.
The system of equations (6.2) is characterized by an impulse response which coincides with the probability density function of the random variable τ, the survival time of a damaged cell. The pdf(τ) so obtained is Erlang(n-1, K1):
wherein K1, t and n are as above defined;
Accordingly, it may be concluded that the convolution integral between the expression (6.4) and the input K2·c(t)·Z1(t) provides the amount of tumor mass which dies in the unity of time.
Model for the tumor Growth in Presence of a Treatment
The overall tumor mass is constituted by the set of cells not damaged by the pharmacological action (able to proliferate according to the equation of growth of the controls) and the set of cells in transit inside the chain of mortality. The overall weight W(t) can be described by the following relationship:
Recalling the equation (5.13), descriptive of the growth of the controls and as underlined in the “chain of mortality” section hereabove, the expression present at the denominator represents a penalty term of the exponential growth of the tumor mass. The damaged tumor mass, even if not participating in the proliferation, contributes to the overall weight since not yet dissolved and should be therefore comprehensive not only of the proliferating mass but of the whole tumor mass; on this ground, the equation (6.1) has to be therefore rewritten in the following way:
The number of compartments inside the chain of mortality in this model was fixed to three. Three compartments inside the chain were sufficient to guarantee a probability density function, having a bell-like shape, of the random variable X and provided also satisfactory results in terms of fitting.
The physiological interpretation of a chain of mortality made of three compartments consists of imagining the “cellular death” event as if it was made discretized in three stages of progressive and irreversible deterioration (the possibility of recovery does not exist), low, medium and high damage which precede the effective death.
Accordingly, the model of tumor growth in vivo can be described by a system of four ordinary differential equations (6.8-6.11′), by the expression (6.6) and by the initial conditions four variables associated to the compartments (zero initial mass for the compartments inside the chain of mortality, L0 for the proliferating compartment):
{dot over (Z)}2(t)=K2·c(t)·Z1(t)−K1·Z2(t) Z2(0)=0 (6.9)
{dot over (Z)}3(t)=K1·Z2(t)−K1·Z3(t) Z3(0)=0 (6.10)
{dot over (Z)}4(t)=K1·Z3(t)−K1·Z4(t) Z4(0)=o (6.11′)
W(t)=Z1(t)+Z2(t)+3(t)+Z4(t) (6.12)
In
Parameters of the Model
The model of growth for the treated subjects, described by the equations (6.8-6.12) requires the use of two further parameters with respect to the four ones adopted in the model for the growth of the controls: K1 and K2 where:
K1 is the parameter which determines the probability density function of the random variable τ, providing indication on the delay between the aggression of the drug and the following cell death. Having fixed the number of compartments inside the chain of mortality, the value of K1 determines in univocal way the time course of the distribution Erlang(3, K1) and, as a consequence, the mean value and the variance of the survival time τ. Dimensionally it represents the inverse of a time, expressed therefore in [day−1]; and
K2 is an index of the capability of the drug to hit and damage tumor cells. It is peculiar of the adopted drug and not of the treated subject. Dimensionally it represents the inverse of a concentration in the unity of time, therefore expressed in [ml g−1 day−1].
In analyzing the experiments A and C, the parameter L0 was not estimated; for each experiment, it was fixed to the average value derived from the control group of each experiment. The values fixed for the two experiments are reported in Tab. 6.1
The shape parameter Ψ remains fixed as in the case of the controls to the value Ψ=20.
Altogether the model of growth in the presence of the drug requires the estimation of the parameters λ0, λ1, K1 and K2.
The fitting of the curve described by the expression (6.8-6.12) was performed, using the set experimental data available for the treated mice in the two experiments A and C, employing the weighted least squares (WLS) as described hereinabove.
Experiment-A: Fitting of the Treated Subjects
The results of the individual fitting for each of the twelve treated mice are shown in Tab. 6.2 and Tab. 6.3. Descriptive statistics (mean, standard deviation and coefficient of variation) of the pharmacodynamic parameters are presented in table 6.4.
The results were then represented graphically in order to compare the observed experimental values of the tumor weight with those predicted by the fitting. Only the results related to four mice (0, 31, 64, 78) of the Experiment-A were represented (see
Experiment-C: Fitting of the Treated Subjects
The estimations of the four parameters of the model related to each of the nine groups of treatment (G2-G10) were computed by the fitting performed on the average curves of growth; the obtained results are shown in Tab. 6.7, while the population values are shown in Tab 6.8.
The observed and predicted values for three of the groups of the Experiment-C are graphically represented in
The proposed model of tumor growth in the presence of a chemotherapeutic treatment provided good results in terms of fitting. The limited number of experimental observations imposed the use of a rather limited number of free parameters for not incurring in problems of model identification. Nevertheless, the bond of structural simplicity required for the model did not prevent from succeeding in describing the time course of the tumor weight in a realistic way, further succeeding in describing the main features underlined by the experimental data. At this regard, a remarkable correspondence between the predicted and observed values during the phase of re-growth of the tumor (delayed after the treatment) has to be noted.
As underlined during the fitting of the two experiments, the present invention allows to describe the experimental data in the short-long term while it is not able to adequately reproduce the time course of the tumor weight in the instants just after the first pharmaceutical treatment. A possible solution involves the use of a pure delay of time between the moment in which the tumor mass is damaged by the aggression of the drug and the instant in which the same one enters in the chain of mortality; the delay of time to be introduced (tlag) allows the tumor mass to have a greater proliferating fraction, allowing a phase of growth even after the first administration. The introduction of the parameter tlag, finds proven theoretical bases (Miklavèiè 1995, Minami 1998, Iliadis 2000) although a clear physiological interpretation did not result.
Number | Date | Country | Kind |
---|---|---|---|
02425157.1 | Mar 2002 | EP | regional |
PCT/EP03/02689 | Mar 2003 | WO | international |