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Chemical Reactor Thermal Runaway Safeguards (Chemical Engineering)

In chemical process engineering, continuous stirred-tank reactors (CSTR) carrying out exothermic autocatalytic polymerizations exhibit nonlinear temperature trajectories. As reactants convert, heat generation accelerates exponentially before flattening as reagents deplete. If the heat-generation rate exceeds cooling jacket dissipation capacity, thermal runaway occurs, causing vessel over-pressurization and explosion.

A process safety engineer is modeling the temperature curve T(t)T(t) (in ∘C^\circ\text{C}) of a batch polymerization reactor over time tt (in hours, t≥0t \ge 0). The temperature response is modeled by the sigmoidal logistic function:

T(t)=50+1201+15e−2tT(t) = 50 + \frac{120}{1 + 15e^{-2t}}

  1. Determine the initial reactor core temperature at startup (t=0t = 0).
  2. Evaluate the horizontal asymptote of the reaction temperature by calculating lim⁡t→∞T(t)\lim_{t \to \infty} T(t). Interpret what this asymptotic temperature represents physically in terms of reagent exhaustion.
  3. Compute the reaction heating rate dTdt\frac{dT}{dt} as a function of time. Show that dTdt>0\frac{dT}{dt} > 0 for all t≥0t \ge 0, proving that core temperature rises monotonically.
  4. Use the Second Derivative Test to locate the time tcritt_{\text{crit}} where the temperature curve has an inflection point (d2Tdt2=0\frac{d^2T}{dt^2} = 0).
  5. In chemical safety design, explain why the inflection point tcritt_{\text{crit}} marks the instant of maximum thermal hazard, dictating the required emergency coolant injection pump capacity.