Skip to main content
Advertisement
Browse Subject Areas
?

Click through the PLOS taxonomy to find articles in your field.

For more information about PLOS Subject Areas, click here.

< Back to Article

Figure 1.

A basic set of two-component homeostatic controller motifs with two implementations of integral control.

(a) Compound is the homeostatic controlled variable and is the controller or manipulated variable [22]. The motifs fall into two classes termed as inflow and outflow controllers, dependent whether their compensatory fluxes add or remove from the system. In motifs outlined in gray the controller compound inhibits the compensatory flux, while in the other motifs activates the compensatory flux. (b) middle figure shows a standard control engineering flow chart of a negative feedback loop, where the negative feedback results in the subtraction of the concentration of (blue line) from 's set-point (red line) leading to the error . The error feeds into the integral controller (brown box). The controller output (the integrated error) is the concentration of (green line) which regulates the process that creates . The perturbations which affect the level of are indicated in orange color. (b) left panel shows the structure of negative feedback (outflow) controller 5. The colors correspond to those of the control engineering flow chart. For example, the set-point (red) is given by the ratio between removing and synthesis rates of , while the integral controller (brown) is related to the processing kinetics of , in this case is removed by zero-order [22], [43]. (b) right panel shows the same outflow controller (motif 5). The only difference is that the integral controller is now represented by a first-order autocatalytic formation (indicated by brown dashed arrow) and a first-order removal with respect to [45].

More »

Figure 1 Expand

Figure 2.

Representation and kinetics of conservative oscillators based on motif 2 and motif 5.

(a)–(c) “Goodwin's oscillator” (motif 2). Conservative oscillations occur when and ; the latter condition introduces integral feedback and thereby robust homeostasis [22], [43]. (b) Conservative oscillations in and , with , , , , , , , . Initial concentrations: , . At time t = 50.0 is changed from 1.0 to 3.0. (c) , , and frequency as a function of the perturbation . While the frequency increases and decreases with increasing , is kept at its set-point . (d)–(f) Harmonic oscillator representation of motif 5. Conservative (harmonic) oscillations occur when (or ) and . (e) Harmonic oscillations in and , with (the perturbation), , , , , , and . At time t = 50.0 is changed from 1.0 to 3.0. Initial concentrations: , . (f) , , and frequency as a function of the perturbation . Typical for the harmonic oscillator is the constancy of the frequency upon changing values. increases with increasing , while is kept at its set-point .

More »

Figure 2 Expand

Figure 3.

A limit-cycle model of controller motif 2.

(a) Reaction scheme. Rate equations: ; ; . (b) Homeostatic response of the model for three different perturbations ( values). For time between 0 and 50 units, , for between 50 and 100 units, , and for between 100 and 150 units, . In the oscillatory case at time is given as (ordinate to the right) showing that is under homeostatic control despite the fact that peak values may be over one order of magnitude larger than the set-point. (c) , , and frequency values as a function of . Simulation time for each data point is 100.0 time units. Note that is kept at independent of . Rate constant values (in au): , , , , , , , and . It may further be noted that the degradation kinetics with respect to are no longer zero-order as required in the conservative case (Figs. 2a–c). Initial concentrations in (b): , , and . Initial concentrations in (c) for each data point: , , and .

More »

Figure 3 Expand

Figure 4.

A limit-cycle model of controller motif 5.

(a). Rate equations: ; ; . (b) Homeostatic behavior in illustrated by three different perturbations ( values). At time is changed from 4.0 to 10.0, and at is changed from 10.0 to 20.0 (indicated by solid arrows). The set-point of is given as . Rate constant values: is variable, , , , , , , and . Initial concentrations: , , and . (c) , , and frequency values as a function of showing that is kept at the set-point independent of . Rate constants as in (b). Initial concentrations for each data point: , , and . Simulation time for each data point is 10000.0 time units.

More »

Figure 4 Expand

Figure 5.

Quasi-harmonic behavior of motif 5 oscillator (Fig. 4a).

For time , a perfect overlay between the numerical calculation of (blue color) and the single harmonic (black color) is found, where , , , , and . and represent the numerically calculated amplitude and period length, respectively. was adjusted to give a closely matching overlay. Other rate constant values (numerical calculations): , , , , , , and . Initial concentrations: , , and . At times and (solid arrows) is changed to respectively 5.0 and 10.0. For these values the amplitude of has reached its maximum, which is twice the value of the set-point. (b) , , , and frequency as a function of . Simulation time for each data point is 1000.0 time units. (c) Demonstration of limit-cycle behavior of the quasi-harmonic oscillations. Same initial conditions as in (a) with , and . (d) Same system as in (a), but at times and (solid arrows) is changed and kept to 0.1. The oscillations are efficiently quenched, but remains under homeostatic control.

More »

Figure 5 Expand

Figure 6.

Oscillator based on motif 5 with robust frequency control.

(a) Reaction scheme. Rate equations: ; ; ; ; . (b) Demonstration of robust frequency control. , , and frequency are shown as functions of . Rate constants: , , , , , , , , , , , , , and . Set-points for by controllers and are given as and , respectively. Initial concentrations for each data point (black dots): , , , , and 2.7657 × 102. Gray dots show the frequency as a function of without control by and . (c) System as in (b), but controller not present. (d) System as in (b), but controller not present. (e) Reaction scheme of oscillator, but with a constant concentration. Rate constants otherwise as in (b). (f) Frequency as a function of for the system described in (e) using different constant concentrations (indicated within the graph). The homeostatic region of the frequency increases with increasing concentrations.

More »

Figure 6 Expand

Figure 7.

Oscillator based on motif 2 with robust frequency control.

(a) Reaction scheme. Rate equations: ; ; ; ; . Shaded area indicates part of the model for which the control coefficents of the frequency/period with respect to the parameters within this area become zero when frequency homeostasis is enforced by controllers and . (b) Demonstration of frequency homeostasis by varying . Black dots show the frequency when controllers and are active. Rate constants: , , , , , , , , , , , , , , , and . Set-points for by controllers and are given as and , respectively. The set-point of the outflow controller has been set slightly higher than for the inflow controller to avoid integral windup and that the controllers work “against” each other [22]. Initial concentrations for each data point (black dots): , , , , and . Gray dots show the frequency as a function of for the uncontrolled case, i.e., in the absence of controllers and . (c) System as in (b), but controller is “knocked out” by setting and to zero. Homeostasis occurs only at high values when controller is active. (d) System as in (b), but inflow controller is inactivated by setting and to zero. Frequency homeostasis is observed for low when controller is active. At high values the frequency homeostasis breaks down, because controller is not present to compensate the increased outflow of , which leads to low values. (e) Oscillations of system in (b) illustrating frequency homeostasis. At time (solid arrow) is changed from 3.0 to 8.0. Initial concentrations: , , , , and .

More »

Figure 7 Expand

Figure 8.

Oscillator based on motif 2 with robust frequency control but alternative feedback regulation by and .

(a) Reaction scheme. Rate equations: , ; ; ; . (b) Using different set-points and , the frequency (solid dots) can switch between two homeostatic frequency regimes, dependent whether is low or high. The two regimes are separated by a transition zone. Rate constants: , , , , , , , , , , , , , . Initial concentrations: , , , , and . (c) Oscillations of system in (b) illustrating frequency switch. At time (solid arrow) is changed from 2.0 to 8.0. Initial concentrations: , , , , and .

More »

Figure 8 Expand

Figure 9.

A limit-cycle model of controller motif 2 using autocatalysis as an integral controller.

(a) Reaction scheme. Rate equations: ; ; . (b) Homeostatic response of the model for three different perturbations ( values). For time between 0 and 250 units, , for between 250 and 500 units, , and for between 500 and 750 units, . at time is defined as in Fig. 3. (c) , , and frequency values as a function of . Simulation time for each data point is 2000.0 time units. Note that is kept at (solid black line) independent of . Rate constant values (in au): , , , , , , and . Initial concentrations in (b): , , and . Initial concentrations in (c) for each data point are the same as in (b).

More »

Figure 9 Expand

Figure 10.

A homeostatic model of cytosolic Ca2+ oscillations.

The model considers a stimulated non-excitable cell under stationary conditions using an extended version of outflow controller motif 6, where is the controller molecule. Intermediate has been included to get limit-cycle oscillations. Rate constant describes the total inflow of Ca2+ from the ER and from the extracellular space into the cytosol and reflects the strength of the stimulation. For the sake of simplicity the external Ca2+ concentration () is considered to be constant ( ). denotes cytosolic Ca2+ and its concentration. (a) Reaction scheme. Rate equations: ; ; . Rate constants: , variable; ; ; ; ; ; . The homeostat's set-point for Ca is given by . (b) oscillations and average cytosolic Ca concentration, , at different stimulations and as a function of time . Initial concentrations: , ; . The quenching of oscillations at low is due to an increased value. (c) Period length and average cytosolic Ca2+ concentration () calculated after 2000 time units for different stimulation strengths ( values). Same rate constants as in (b) with . Initial concentrations for each calculated data point: , ; .

More »

Figure 10 Expand