Why Sampling Time Must Follow the Input Profile
A sample can be analytically precise yet contribute little to the parameter of interest. For an oral dose with an absorption lag, a measurement taken well after the concentration peak may describe elimination clearly but provide weak information about when absorption began. Conversely, an early sample close to the lag can be highly sensitive to lag time, but that advantage depends on knowing the lag closely enough to schedule the sample on the intended side of onset.
Transit absorption creates a different timing problem. Rather than a single sharp onset followed by first-order absorption, a sequence of transit compartments spreads drug input over time. The sampling plan should therefore distinguish the beginning of the input profile, its central region, and the later concentrations shaped primarily by absorption and elimination. The objective is not to sample at one universally “best” time: it is to obtain complementary information about the parameters the individual model is intended to estimate.
Lag-Time Model and Local Information
Consider a one-compartment oral model with first-order absorption and elimination, a lag time \(L\), and additive concentration error. Let \(u=t-L\) denote time since the lag has elapsed. For \(t>L\), write the concentration as
where \(k_a\) and \(k_e\) are the absorption and elimination rate constants, respectively, and \(B\) is a positive concentration scale. For \(t\leq L\), the model prediction is zero. Assume \(k_a>k_e>0\), a fixed dose, a correctly specified model, and observation errors that are independent Gaussian errors with mean zero and known variance \(\sigma^2\). For local sensitivity calculations, treat \(B\), \(k_a\), and \(k_e\) as fixed while assessing information about \(L\).
Because \(u=t-L\), differentiating with respect to \(L\) is the negative of differentiating with respect to \(u\). Thus,
This derivative explains why samples at different phases have different roles. Before the lag, the prediction is constant at zero, so its ordinary local derivative with respect to \(L\) is zero. Just after onset, the concentration can change rapidly when \(L\) shifts, making the derivative large in magnitude. At the concentration peak, the time derivative is zero, so the lag-time derivative is also zero. Later, the absorption contribution fades and the lag sensitivity generally becomes smaller.
For several independent samples at times \(t_i\), with the same error variance, the scalar information for \(L\) is
This is local information: it describes curvature around a specified nominal value of \(L\) and the other model parameters. It is not a guarantee that the estimate will be precise if the nominal model is wrong or the data do not support the assumed error structure.
Worked Example: Information From a Sample Just After the Lag
Suppose a hypothetical oral PK model has \(B=12.0\) mg/L, \(k_a=1.20\) h\(^{-1}\), \(k_e=0.200\) h\(^{-1}\), and nominal lag \(L=0.500\) h. A sample is scheduled at \(t=0.600\) h, so \(u=0.100\) h. Assume the additive residual standard deviation is \(\sigma=0.500\) mg/L, and all parameters except \(L\) are treated as fixed for this calculation.
The sensitivity is
Substituting the exponentials gives
The one-sample local information is therefore
The negative sign means that, at this time and nominal parameter values, increasing the lag decreases the predicted concentration. Information itself is nonnegative because it uses the squared sensitivity. The large local value reflects the steep change near onset; it should not be interpreted as proof that this time is robustly optimal when the true lag is uncertain.
Transit Absorption: A Distributed Input
A standard transit model represents absorption input as the output of a sequence of transit compartments. Let \(n\) be the number of transit compartments before the absorption depot, and let \(k_{\mathrm{tr}}\) be the common transit rate constant. The transit delay density is a gamma density:
It integrates to one, has mean transit time \(\mathrm{MTT}=(n+1)/k_{\mathrm{tr}}\), and, for \(n\geq1\), has its mode at \(n/k_{\mathrm{tr}}\). These describe the distribution of transit delays, not the time of the plasma concentration peak. After the transit delay, first-order absorption and elimination further shape the concentration.
For example, with a lag \(L\), the concentration can be expressed as the transit density convolved with the one-compartment response to a dose entering the absorption depot:
Here \(F\) is bioavailability and \(V\) is apparent volume. The transit profile broadens input, so sampling only at an anticipated sharp onset is less compelling than in a simple lag model. Useful times typically span the early rise, the central input region, and a later declining period. The precise concentration peak depends on transit, absorption, and elimination together; it cannot be read directly from the transit-density mode.
Worked Example: Locating the Central Transit Region
Consider a hypothetical model with \(n=2\) transit compartments and \(\mathrm{MTT}=1.50\) h. The rate is
The delay density is \(g_2(s)=4s^2e^{-2s}\), with \(s\) measured in hours and \(g_2\) in h\(^{-1}\). Its mean is 1.50 h, while its mode is
At \(s=0.500\) h, \(g_2(s)=4(0.500)^2e^{-1}\approx0.3679\) h\(^{-1}\). At \(s=1.00\) h, \(g_2(s)=4e^{-2}\approx0.5413\) h\(^{-1}\). At \(s=2.00\) h, \(g_2(s)=16e^{-4}\approx0.2931\) h\(^{-1}\). These values show that the transit delay density is largest near 1.00 h and is still appreciable on either side.
A reasonable initial schedule for evaluating the predicted concentration might therefore include samples before or near the beginning of input, around the central rise, and after that rise. The 1.00 h delay-density mode is a guide to where input delays concentrate, not a calculated concentration-peak time. The latter requires the full convolution with \(k_a\) and \(k_e\), and the sample schedule should be checked against the full model predictions and sensitivities.
Onset, Peak, and Post-Absorption Samples
The timing distinction is particularly clear in the lag model. The concentration peak occurs at time \(t_{\max}=L+u_{\max}\), where setting the time derivative to zero gives
At this time, \(\partial C/\partial L=0\): moving the lag shifts the whole profile horizontally, but a sample exactly at the profile’s maximum has no first-order change in its predicted concentration under a small lag shift. A peak sample can still help estimate scale or other parameters; it is specifically weak for local lag information. Samples on the declining limb can inform elimination, while very late samples may contain little information about absorption because the absorption exponential has nearly vanished.
Worked Example: Comparing Early, Peak, and Late Lag Sensitivity
Use the hypothetical values \(B=12.0\) mg/L, \(k_a=1.20\) h\(^{-1}\), \(k_e=0.200\) h\(^{-1}\), \(L=0.500\) h, and \(\sigma=0.500\) mg/L. The peak occurs at
At \(u=0.100\) h, the predicted concentration is \(12.0(e^{-0.0200}-e^{-0.120})\approx1.119\) mg/L, and the sensitivity is approximately \(-10.4192\) (mg/L)/h, giving \(434.2\) h\(^{-2}\) of local information. At \(u=u_{\max}\), the derivative is zero by the peak condition, so the one-sample local information for \(L\) is zero.
For a later sample at \(u=4.00\) h, the concentration is \(12.0(e^{-0.800}-e^{-4.80})\approx5.293\) mg/L. Its lag sensitivity is
The corresponding information is \((0.9599)^2/(0.500)^2\approx3.686\) h\(^{-2}\). In this local calculation, the near-onset sample is much more informative about \(L\) than the peak or late sample. In a multi-parameter design, however, complementary times may be needed to distinguish \(L\) from rate constants and scale.
Assumptions, Diagnostics, and Design Choices
The calculations above assume a correct structural model, known nominal parameter values, accurately recorded sampling times, and independent Gaussian additive errors with constant known variance. The local information formula follows from the derivative of the model mean under those assumptions. If assay variability changes with concentration, the variance in the information calculation must reflect that error model; if observations are correlated, summing independent one-sample contributions is not valid.
A lag estimate can be fragile when a sample is scheduled very close to nominal onset. A small error in actual dose time, sample time, or nominal \(L\) can move the observation from just after onset to before it. Moreover, at exactly \(t=L\), the piecewise model is not smoothly differentiable in the ordinary two-sided sense. Do not use the steep post-lag derivative as if it applied across the boundary.
Useful diagnostics include plotting predicted concentrations and parameter sensitivities against time, checking whether the proposed samples fall on the intended side of the nominal lag, and recomputing the design over plausible values of \(L\), \(k_a\), and \(k_e\). If the high-information time shifts substantially across plausible values, include samples that bracket the onset rather than relying on one narrowly timed draw. For transit models, inspect both the transit density and the full predicted concentration profile; the former alone does not establish where concentration information is greatest.
A peak-focused schedule is easy to motivate when the clinical interest is maximum concentration, but it is a poor stand-alone strategy for lag estimation. Evenly spaced samples are less dependent on a single nominal peak or onset, though they may spend draws in uninformative regions. A sensitivity-based schedule targets parameter information directly; in practice, it should be balanced across parameters and checked for robustness. None of these approaches removes the need to consider feasible clinic windows, assay limits, or model misspecification.
Check Your Understanding
Answer each question, then compare your reasoning with the brief solutions.
- In a first-order absorption model with lag, why is an exact peak sample locally uninformative about \(L\)?
- For \(n=3\) transit compartments and \(\mathrm{MTT}=2.00\) h, calculate \(k_{\mathrm{tr}}\) and the transit-density mode.
- With additive error standard deviation \(\sigma\), how does one-sample information change if the absolute sensitivity doubles?
- Why can a sample scheduled just after a nominal lag be a fragile design choice?
- Does the mode of the transit-delay density necessarily equal the plasma concentration peak? Explain.
Solutions. (1) At the peak, the concentration’s time derivative is zero; lag shifts the profile in time, so its local derivative with respect to \(L\) is also zero. (2) \(k_{\mathrm{tr}}=(3+1)/(2.00\ \mathrm{h})=2.00\) h\(^{-1}\), and the mode is \(n/k_{\mathrm{tr}}=3/2.00=1.50\) h. (3) Since information is sensitivity squared divided by \(\sigma^2\), doubling absolute sensitivity multiplies information by four. (4) Small errors in lag, dose time, or sample time can place the actual sample before rather than after onset, where the ordinary post-lag sensitivity formula does not apply. (5) No. The density mode describes transit delays; the plasma concentration peak also depends on absorption and elimination through the full input-response convolution.