Gas Fraction Drives
the Gas Scale.
81% Within 20%.
Replacing a fixed gas scale with one that transitions smoothly from stellar-tied ($1.7\,R_d$) to HI mass-based ($R_\text{HI}/6.1$) as gas fraction increases — controlled by a sigmoid with centre $f_\text{gas}=0.68$ — improves the prediction from 74% → 81% within 20% of $V_f$. Only 4 galaxies exceed 50% error, all ultra-compact pure-gas dwarfs with $R_d < 0.7\,\text{kpc}$.
The Pearson correlation between predicted and observed velocities jumps to r = 0.966 from 0.941. The median error drops to 10.4%. This is achieved by adding two physically motivated parameters: the gas fraction at the stellar-to-HI transition ($w_c = 0.68$) and the HI effective scale factor ($f_f = 6.1$).
128 / 159
↓ from 11.3%
↑ from 0.941
36 / 40 within 20%
152 / 159
all $R_d < 0.7$ kpc
1. The prediction — 159 galaxies
2. The key change — adaptive gas scale
The single innovation in v3 is a gas ring scale $R_g$ that depends on the gas fraction $f_\text{gas}$. For stellar-dominated galaxies ($f_\text{gas} \ll 0.68$) it reduces to the old $1.7\,R_d$. For gas-dominated galaxies ($f_\text{gas} \gg 0.68$) it transitions smoothly to a scale derived from the HI mass–radius relation.
$w_c = 0.678$: the gas fraction where the gas source transitions from stellar-disk tied to HI-mass based. Below this value, the stellar disk defines the gas ring scale. Above it, the HI extent dominates.
$f_f = 6.09$: converts the Wang et al. outer HI radius, measured at the $1\,M_\odot/\text{pc}^2$ isodensity, to the effective BeeTheory ring scale.
$k = 10$: controls the transition sharpness. It is fixed, not optimised, and results are stable for $k$ between about 6 and 15.
3. Complete parameter table
Unchanged from v1
New in v3 — gas geometry
$w_c$ and $f_f$ are the only parameters introduced in v3. All other parameters remain fixed from the Milky Way calibration and the original 20-galaxy SPARC fit.
4. Remaining 4 outliers
| Galaxy | $V_f$ | $V_\text{BT}$ | Error | $f_\text{gas}$ | $R_d$ | $w$ | $R_g$ | Why |
|---|---|---|---|---|---|---|---|---|
| DDO064 | 26 | 44 | +70% | 0.85 | 0.33 | 0.84 | 1.12 | Ultra-compact. $R_d = 0.33$ kpc. HI surface density profile needed. |
| KK98-251 | 17 | 31 | +83% | 0.74 | 0.30 | 0.65 | 0.51 | Extremely small galaxy. At $V_f=17$ km/s, measurement uncertainty is large. |
| ESO444-G084 | 27 | 45 | +66% | 0.74 | 0.55 | 0.64 | 0.99 | Gas-dominated irregular. No exponential stellar disk. |
| NGC3741 | 51 | 77 | +52% | 0.72 | 0.68 | 0.62 | 1.85 | Very extended HI relative to stars. Per-galaxy 21 cm profile needed. |
All four outliers have $R_d < 0.7\,\text{kpc}$, $f_\text{gas} > 0.70$, and irregular morphologies. In these systems, the exponential stellar disk model has limited physical meaning: the galaxy is dominated by gas. The correct BeeTheory source is the measured HI surface density profile $\Sigma_\text{HI}(R)$ from 21 cm maps.
MOND achieves roughly 85% within a factor of 1.5 on SPARC using one free parameter, $a_0$. BeeTheory v3 achieves 96% within 35%, using adaptive gas geometry while keeping the fundamental coupling $K_0$ fixed across galaxy types and scales.
Data: Lelli et al. AJ 152, 157 (2016) · HI radius: Wang et al. MNRAS 460, 2143 (2016) · HI scale: Swaters et al. (2009) · BeeTheory: Dutertre (2023), extended 2025 · $K_0$, $c_\text{disk}$, $c_\text{sph}$ fixed from MW + original 20-galaxy calibration · $w_c$, $f_f$ fitted on 159-galaxy sample