Problem 1 — Full dynamics vs Michaelis-Menten
From the data table: V₀ = Vmaxs₀/(Km+s₀) fits exactly with Vmax = 5 mM/min (the one correct statement) and Km = 3 mM. With e₀ = 10 mM: k₂ = Vmax/e₀ = 0.5/min, and using kf = 10kr in Km = (kr+k₂)/kf: kf ≈ 0.172/min, kr ≈ 0.0172/min. The three ODEs: ds/dt = −kf e s + krc, dc/dt = kf e s − (kr+k₂)c, dp/dt = k₂c, with e = e₀−c.
Why the curves differ: Michaelis-Menten assumes the complex C is in quasi-steady state and that s ≈ s₀ initially. During the first fraction of a minute (left plot) the complex is still forming, so the MM product curve leads the true one; late in the reaction substrate depletion makes both converge.
Problem 2 — Determine Km by inspection, then simulate
Vmax = 6.0 µM/s. The data row V₀ = 3.0 µM/s (= ½Vmax) occurs at [S]₀ = 100 mM — so Km = 100 mM with no calculation needed. Drag the Km slider and watch the curve pass through the data.
Problem 4 — Lineweaver-Burk plot with an inhibitor
1/V = (Km/Vmax)(1/[S]) + 1/Vmax. Both datasets are fitted live by least squares. The two lines come out nearly parallel (slope ratio ≈1.3 — for real experimental data that difference is unlikely to be significant), while Vmax and Km both fall by about the same factor (≈3×). Parallel Lineweaver-Burk lines with proportionally reduced Vmax and Km are the signature of uncompetitive inhibition: the inhibitor binds only the ES complex, so adding more substrate produces more complex to inhibit — the inhibition cannot be overridden by extra substrate.
Problem 5 — PFK-1: Michaelis-Menten or Hill?
The experimental curve is sigmoidal (slow start, then steep rise) — that is Hill dynamics, i.e. cooperative binding: V = Vmax[S]n/(Kn+[S]n). Adjust the sliders to fit the data; the best MM fit (dashed) can never reproduce the sigmoid foot at low [S].