Bacterial Density, Phage Half-Life, Transit Times, and MOI within Biofilms
by Stephen T. Abedon Ph.D. (abedon.1@osu.edu)
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Version 2026.04.07
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Enter the surface cell density and biofilm height to estimate the volumetric bacterial concentration within the biofilm. This density is the key quantity linking biofilm structure to phage adsorption kinetics, and is automatically passed to Sections 2 and 4.
The time for half a phage population to adsorb bacteria is t½ = ln(2) / (k × N), where k is the adsorption rate constant and N is the bacterial density (auto-filled from Section 1). A smaller half-life means phages adsorb bacteria more rapidly. Note that the manually entered k above is used as-is for the primary half-life result; use the Smoluchowski panel below to explore how matrix-reduced diffusion modifies kadj and its corresponding half-life. For a direct phage half-life calculator see t05phage.phage.org. For a theoretical estimate of k see adsorption.phage.org.
The adsorption rate constant can be expressed as k = 4πRDαf, where R is the effective encounter radius, D is the phage diffusion coefficient, α is a scaling factor representing reduction in D within the biofilm matrix (default 1.0 = free solution), and f is the probability of successful adsorption upon encounter. The diffusion-adjusted rate constant is denoted kadj = 4πRDαf; when α = 1.0, kadj reduces to the standard Smoluchowski expression. Adjusting α below 1.0 simulates the effect of matrix-impeded diffusion on kadj and hence on phage half-life. The D value used here is linked to Section 3.
Phages move through a biofilm by diffusion, not by directed transport. The distribution of times for a single phage to traverse the full biofilm thickness L (auto-filled from Section 1) follows a first-passage time distribution — skewed, with a long tail toward slow crossings. Two quantities characterize this distribution: the modal transit time (the most probable, and also the fastest realistically expected, crossing time, = L² / 6D) and the mean transit time (the average crossing time, = L² / 2D), which is exactly three times the mode. The half-life from Section 2 captures the competing process of adsorption occurring during transit.
Reducing α below 1.0 scales D to simulate matrix-impeded diffusion within the biofilm. This affects both the transit time calculations below and the Smoluchowski-derived kadj in Section 2 — both panels share the same α value.
Convert between common diffusion coefficient units.
The multiplicity of infection (MOI) is the ratio of phage to bacteria. Within a biofilm, the relevant bacterial density is the volumetric concentration estimated in Section 1 — auto-filled below. Enter the phage titer (PFU ml−1) to compute the MOI within the biofilm. For Poisson-based MOI calculations see also moi.phage.org.
A biofilm is a structured community of bacteria usually found attached to a surface, encased in a self-produced extracellular matrix. Unlike planktonic bacteria suspended in liquid culture, biofilm bacteria are densely packed in three dimensions. The volumetric bacterial density within a biofilm can be estimated from two measurable quantities: the number of cells per unit area (from surface counts or microscopy) and the biofilm height or thickness (from confocal imaging or profilometry).
The conversion is straightforward: dividing the surface cell density (cells per area) by the biofilm height (length) gives a volumetric density (cells per volume). For example, Hamilton (1987) reported a surface density of 5 × 107 cells cm−2 and a biofilm height of 150 μm in an oil-field pipeline biofilm:
This density — roughly 3 billion bacteria per milliliter — is comparable to or somewhat higher than typical late-log or stationary-phase planktonic cultures. Importantly, biofilm density varies widely across biofilm types, ages, species, and substrates; this calculator is useful precisely for estimating what the actual volumetric density is for a given biofilm, rather than assuming a typical value. The calculated density feeds directly into the phage adsorption and MOI calculations in the Calculator tab.
Note that this calculation yields an average density across the full biofilm volume. Real biofilms are heterogeneous; local densities vary, and not all bacteria within a biofilm may be of the same species or phage-susceptibility type. At spatial scales of 10–100 μm, however, clonal microcolonies mean that local densities of susceptible bacteria can be reasonably approximated by this average as a first estimate.
Phage adsorption follows first-order kinetics with respect to both phage and bacterial concentrations. The rate constant k (the adsorption rate constant) has units of volume per time (typically ml min−1). The half-life of the phage population — the time for half the phages to adsorb — is:
Using k = 2.5 × 10−9 ml min−1 (Stent, 1963) and the Hamilton (1987) biofilm density of 3.3 × 109 cells ml−1, the phage half-life is approximately 0.084 minutes — less than 5 seconds. This represents the expected time for half a phage population to adsorb bacteria under these conditions, and is a lower bound: to the extent that phage diffusion is reduced within the biofilm matrix (see below), the effective adsorption rate constant and hence the encounter rate will also be reduced, lengthening the actual half-life. See t05phage.phage.org for a dedicated phage half-life calculator.
Stent's (1963) value of k = 2.5 × 10−9 ml min−1 applies to phage T4 adsorbing E. coli under standard conditions. Values of k for other phage-host pairs can be higher (e.g., 10−9 ml min−1 and above) as well as somewhat lower (e.g., 10−10 ml min−1 and below). For a theoretical estimate of k from first principles, see adsorption.phage.org.
The adsorption rate constant is not independent of the phage diffusion coefficient. From Smoluchowski theory, k = 4πRDf, where R is the effective encounter radius (approximated by bacterial radius, ~1 μm), D is the phage diffusion coefficient, and f is the probability of successful adsorption given encounter (0–1). Because k scales linearly with D, any reduction in phage diffusion within the biofilm matrix — through steric hindrance by the extracellular matrix and bacterial cells — directly reduces k and therefore lengthens both phage half-life and phage transit time. The calculator allows the user to explore this relationship by adjusting a scaling factor α that multiplies D, giving kadj = 4πRDαf.
Phages are not actively motile; they move through a biofilm entirely by diffusion. The relevant physical quantity is the diffusion coefficient D, which relates mean squared displacement to time: ⟨x²⟩ = 2Dt in one dimension.
For phage T4 in free solution, Stent (1963, citing Putnam, 1954) gave D = 2.4 × 10−6 cm² min−1, equivalent to approximately 4.0 μm² s−1. Hunter et al. (2021) measured D0 = 4.13 ± 0.19 μm² s−1 for phage T7 (a podovirus) in free solution — close to but somewhat faster than the T4 value, consistent with T7's smaller size giving a modestly higher diffusion coefficient (Stokes-Einstein: D ∝ 1/r).
Within a biofilm matrix, however, phage diffusion is impeded by steric interactions with the bacterial matrix. Hunter et al. (2021) showed that phage T7 diffusion in a bacterial lawn follows Fricke's law, with D decreasing substantially as bacterial density increases. At high bacterial densities comparable to those in biofilms, D can be reduced by an order of magnitude or more relative to free solution — and because k scales linearly with D (Smoluchowski), this reduction in diffusion also lengthens the phage half-life. The transit time calculations in Section 3 use an effective diffusion coefficient Deff = α × D, where α can be adjusted to simulate matrix impedance.
The distribution of first-passage times for a particle diffusing across a slab of thickness L is not symmetric — it has a long tail toward slow crossings. Two useful summary statistics are:
The mean is exactly three times the mode. Both are finite and meaningful; the distribution ranges from near-zero (rare fast crossings) to very long (rare slow crossings). Together with the half-life from Section 2, these transit times give a sense of whether phages are likely to traverse the full biofilm depth before being adsorbed.
The multiplicity of infection (MOI) is the ratio of phage particles to bacteria. In planktonic culture, the relevant bacterial density is simply the culture density. In a biofilm, the relevant density is the volumetric bacterial concentration within the biofilm — which may differ substantially from the density of any surrounding liquid. An MOI calculated using the biofilm bacterial density therefore reflects the local phage-to-bacterium ratio experienced by bacteria within the biofilm. See moi.phage.org for a Poisson-based MOI calculator, adsorptions.phage-therapy.org for adsorption-based dose calculations, and t05phage.phage.org for phage half-life calculations.
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