SIAM News Blog
Research

The Golden Ratio for Cortisol Replacement

<strong>Figure 1.</strong> Schematic of hormone production stimulation in the hypothalamus-pituitary-adrenal (HPA) axis. Figure courtesy of Rosie Evans.
Figure 1. Schematic of hormone production stimulation in the hypothalamus-pituitary-adrenal (HPA) axis. Figure courtesy of Rosie Evans.

Cortisol, one of the body’s main stress hormones, is primarily responsible for glucose metabolism and immune system regulation. The hypothalamus-pituitary-adrenal (HPA) axis regulates the levels of cortisol in the body (see Figure 1) [4]. Individuals with primary adrenal insufficiency (PAI) are unable to produce a sufficient quantity of cortisol, leading to symptoms such as weight loss, muscle weakness, and low blood pressure [1]. PAI treatment typically involves the use of synthetic cortisol—delivered via continuous intravenous (IV) infusion, repeated IV bolus injection, or in the form of a tablet—to replace what the body cannot make. But since both the quantity and method of treatment affect the resulting levels of hormone in the blood, the optimization of cortisol replacement for individual patients is a complex task. By mathematically modeling the HPA axis, we aim to simulate various treatment regimens to enable the prediction of different (optimal) strategies.

We begin with a single-compartment pharmacokinetic model that builds upon an existing model [3] to estimate concentrations of cortisol in different parts of the body (see Figure 2). Free cortisol—in the form of hydrocortisone—is administered into the blood, where it can bind to proteins or be removed (i.e., metabolized or excreted) from the system. We can write this model with mathematical equations that represent the change in the levels of free cortisol and binding protein over time (derivatives with respect to \(t\)):

\[\frac{dF_f}{dt}= \alpha q(t) - k_{fb}F_fB + k_{bf}F_b - k_{re}F_f, \tag1\]

\[\frac{dB}{dt}= - k_{fb}F_fB + k_{bf}F_b, \tag2\]

\[\frac{dF_b}{dt}= + k_{fb}F_fB - k_{bf}F_b. \tag3\]

<strong>Figure 2.</strong> The single-compartment pharmacokinetic model that estimates cortisol concentrations in different parts of the body. Here, \(\alpha\) is a dilution factor for the hydrocortisone dose as it enters the blood. Figure courtesy of Rosie Evans.
Figure 2. The single-compartment pharmacokinetic model that estimates cortisol concentrations in different parts of the body. Here, \(\alpha\) is a dilution factor for the hydrocortisone dose as it enters the blood. Figure courtesy of Rosie Evans.

The key considerations that underly this model are (i) the binding protein (corticosteroid-binding globulin)’s high affinity for free cortisol and (ii) the fact that only free cortisol can be removed from the system. The following initial conditions are also present:

\[F_f(0)=0, \;\;\;\; B(0) = B_0,\]

\[F_b(0) = 0, \tag4\]

where \(B_0\) is the physiological level of binding protein. We assume that the amount of cortisol in a patient with adrenal insufficiency is negligible (a simplification that we will further consider in the future). Here, \(q(t)\) is a known input of the drug dose. We have three state variables—free cortisol \((F_f)\), bound cortisol \((F_b)\), and unoccupied binding protein \((B)\)—as well as five unknown parameters \((\alpha,\) \(k_{fb},\) \(k_{bf},\) \(k_{re},\) and \(B_0)\) that we wish to fit via patient data. By eliminating bound cortisol, we can reduce the model to a system of two ordinary differential equations (ODEs):

\[\frac{dF_f}{dt}=\alpha q(t)- k_{fb}F_fB + k_{bf}(B_0-B) - k_{re}F_f, \tag5\]

\[\frac{dB}{dt}= - k_{fb}F_fB + k_{bf}(B_0-B). \tag6\]

Temporal Evolution of Cortisol

Solving the ODE model reveals the way in which the free cortisol and binding protein concentrations change throughout a single high-dose period (see Figure 3). To do so, we model an IV bolus as a high dose that is delivered continuously over a one-minute period, i.e.,

\[ q(t) = \begin{cases}
                q, & 0\leq t\leq1\\
                0, & 1<t. 
            \end{cases} \tag7\]

During dosing, the binding protein and cortisol quickly bind, thereby reducing the level of free cortisol. In this high-dose case, the binding protein is almost completely saturated by the end of the dosing period; once dosing concludes, free cortisol is eliminated and removed from the system. Binding and unbinding occur continuously, which leads to a slow increase in the binding protein. Eventually, all cortisol is removed.

&lt;strong&gt;Figure 3.&lt;/strong&gt; The full (dimensional) system solution for a high-dose scenario. Figure courtesy of Rosie Evans.
Figure 3. The full (dimensional) system solution for a high-dose scenario. Figure courtesy of Rosie Evans.

Rational Model Simplification

Based on small amounts of empirical data, we assume that binding is the fastest process in the system, followed by unbinding [2]. These two processes each occur on much shorter timescales than the dosing period of one minute, which is still significantly faster than the removal rate (see Figure 4). This insight allows us to simplify the model and will facilitate parameter estimation when we ultimately fit our model to data, as it can reduce and simplify the equations we want to solve and/or reduce the number of unknown parameters we seek to estimate.

&lt;strong&gt;Figure 4.&lt;/strong&gt; Hierarchy of the speed of processes in the system. Figure courtesy of Rosie Evans.
Figure 4. Hierarchy of the speed of processes in the system. Figure courtesy of Rosie Evans.

A Fun Aside: The Golden Ratio Emerges

We now break the full solution into three different regions as free cortisol and the binding protein interact. By separating the rates, we see that binding is the dominant process in the dosing period. Initially, the binding protein is saturated by incoming free cortisol (see “Initial Binding” in Figure 5). Once the protein is mostly saturated, the amount of free cortisol rises steadily (see “Increase in \(F_f\)" in Figure 5). We want to find a combination of solutions that will match the entire dosing period, so we look for a third crossover region to bridge the gap between the other two solutions (see “Crossover” in Figure 5). Within this region, we see that the level of unoccupied binding protein crosses through a value that is proportional to the golden ratio (circled in gold in Figure 5). In dimensional variables, 

\[B = B_0 \delta^\frac{1}{2} \left({\color{gold}{\frac{1+\sqrt{5}}{2}}}\right) \quad \text{at} \quad t = \frac{B_0\tau}{\alpha D}\left(1-\left(\frac{k_{bf}}{k_{fb}B_0}\right)^\frac{1}{2}\right).\]

&lt;strong&gt;Figure 5.&lt;/strong&gt; Comparison of the full and simplified systems during the dosing period. Figure courtesy of Rosie Evans.
Figure 5. Comparison of the full and simplified systems during the dosing period. Figure courtesy of Rosie Evans.

After delivery of the dose, we can reduce the model to a single equation that describes the remainder of the time (see Figure 6). We begin by defining a new variable \(x\) for the difference between the two variables \((x=F_f-B)\). This new variable allows us to eliminate \(F_f\) from the system and obtain a novel pair of ODEs with one slow and one fast variable. From this new system, we then take an asymptotic expansion and equate coefficients to find an ODE for the slow manifold solution of \(x\). The resulting single equation describes the unbinding and the gradual removal of cortisol, with protein returning to pre-dosing levels. Notably, the golden ratio appears again as the binding protein increases:

\[B = B_0\delta^\frac{1}{2}\left(1-\frac{\delta^\frac{1}{2}}{\sqrt{5}}\right)\left({\color{gold}{\frac{1+\sqrt{5}}{2}}}\right).\]

With this approach, we aim to fit the simplified model to patient response data and estimate model parameters. The model reductions allow us to solve the system much more quickly, which will assist with parameter inference. In the long term, we hope to test different treatment strategies to determine what works best for a particular individual. This effort is particularly important for patients who undergo other stressors, as their dosing amounts may consequently require alterations.

&lt;strong&gt;Figure 6.&lt;/strong&gt; Comparison of the full and simplified systems after the dosing period. Figure courtesy of Rosie Evans.
Figure 6. Comparison of the full and simplified systems after the dosing period. Figure courtesy of Rosie Evans.

Rosie Evans delivered a contributed presentation on this research at the 2023 SIAM Conference on Applications of Dynamical Systems (DS23), which took place in Portland, Ore., in May 2023. She received funding to attend DS23 through a SIAM Student Travel Award. To learn more about Student Travel Awards and submit an application, visit the online page

SIAM Student Travel Awards are made possible in part by the generous support of our community. To make a gift to the Student Travel Fund, visit the SIAM website

Acknowledgements: The authors would like to thank Wiebke Arlt and her team at the University of Birmingham for providing the data around which this work is based.

References
[1] Charmandari, E., Nicolaides, N.C., & Chrousos, G.P. (2014). Adrenal insufficiency. Lancet, 383(9935), 2152-2167.
[2] Picard-Hagen, N., Gayrard, V., Alvinerie, M., Smeyers, H., Ricou, R., Bousquet-Melou, A., & Toutain, P.L. (2001). A nonlabeled method to evaluate cortisol production rate by modeling plasma CBG-free cortisol disposition. Am. J. Physiol. Endocrinol. Metab., 281(5), E946-E956.
[3] Smith, D.J., Prete, A., Taylor, A.E., Karavitaki, N., & Arlt, W. (2020). Modelling oral adrenal cortisol support. Preprint, arXiv:2006.00043.
[4] Zavala, E., Wedgwood, K.C.A., Voliotis, M., Tabak, J., Spiga, F., Lightman, S.L., & Tsaneva-Atanasova, K. (2019). Mathematical modelling of endocrine systems. Trends Endocrinol. Metab., 30(4), 244-257.

About the Authors

Rosie Evans

University of Birmingham

Rosie Evans recently completed her Ph.D. at the University of Birmingham, where she worked in the Mathematical Biology Group under the supervision of Meurig Gallagher and David Smith. Her research focuses on endocrinology and mathematical modeling, with a particular interest in parameter identifiability and model reduction through matched asymptotic analysis. She is also a former co-lead of The Piscopia Initiative, an international network of women and underrepresented genders within mathematical research.

Meurig T. Gallagher

Assistant professor, University of Birmingham

Meurig T. Gallagher is an assistant professor and the Human Fertilisation and Embryology Authority Research Person Responsible at the University of Birmingham. He is the Basic Science Officer for the European Society of Human Reproduction and Embryology’s Special Interest Group for Andrology and sits on the Executive Committee of the Association of Reproductive and Clinical Scientists. Gallagher integrates mathematical modeling and software with experimental methods to create new diagnostics and treatments for subfertility, using a comprehensive interdisciplinary approach to tackle wider healthcare applications.

David J. Smith

Professor, University of Birmingham

David J. Smith is a professor of applied mathematics at the University of Birmingham. He is also editor-in-chief of the journal Mathematics in Medical and Life Sciences and leads the U.K. Fluid Network’s Special Interest Group in Biologically Active Fluids. Smith has over 20 years of experience in the development of physiological models in close collaboration with researchers in biomedicine and healthcare. He holds particular interests in reproduction, development, and endocrinology.