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MS/PhD Reactor Safety: Throughput Increase and Runaway Risk

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MS/PhD Reactor Safety: Throughput Increase and Runaway Risk

A chemical engineering MS candidate reviews a proposal to increase throughput in a 2 m³ jacketed CSTR. The reactor processes an aqueous first-order exothermic reaction A → B. Current feed is 1.0 m³ h⁻¹ with C_A0 = 2.0 kmol m⁻³ at 300 K. At the desired 80% conversion the reactor operates at 350 K. The reaction enthalpy is −80 kJ mol⁻¹, the activation energy is 60 kJ mol⁻¹, and the mixture has ρ = 1000 kg m⁻³ and c_p = 4.0 kJ kg⁻¹ K⁻¹. The jacket uses coolant at 300 K and at maximum flow provides UA = 1.0 kW K⁻¹. The proposal raises C_A0 to 3.0 kmol m⁻³ while keeping feed rate, conversion, and coolant conditions unchanged. The candidate must assess the steady-state and runaway risks, not just the extra heat release.

1. Calculate the heat release and adiabatic temperature rise for the current and proposed feeds at 80% conversion.

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Current feed: F_A0 = 1.0 × 2.0 = 2.0 kmol h⁻¹. At 80% conversion, 1.6 kmol h⁻¹ reacts. Q_dot = 1.6 × 80,000 = 128,000 kJ h⁻¹ = 35.6 kW. ΔT_ad = Q_dot / (ρ Q c_p) = 128,000 / [1000(1.0)(4.0)] = 32 K.

Proposed feed: F_A0 = 3.0 kmol h⁻¹, reacted = 2.4 kmol h⁻¹. Q_dot = 2.4 × 80,000 = 192,000 kJ h⁻¹ = 53.3 kW. ΔT_ad = 48 K.

The adiabatic rise is 50% larger.

2. At 350 K, what is the maximum heat removal rate? Can the proposed feed be steady at 350 K? If not, predict the direction of temperature change and explain the feedback.

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At 350 K with coolant at 300 K: Q_rem = UA(350 − 300) = 1.0(50) = 50 kW.

Current generation 35.6 kW < 50 kW, so at 350 K the jacket has excess capacity; coolant flow would be throttled. Proposed generation 53.3 kW > 50 kW, so 350 K cannot be steady at full cooling. The temperature must rise.

As T rises, the Arrhenius rate constant increases, so heat generation rises roughly exponentially, while removal rises only linearly with T. The slope of generation at 350 K is approximately Q_gen E_a/(R T²) = 53.3(60,000)/[8.314(350)²] ≈ 3.1 kW K⁻¹, compared with the removal slope UA = 1.0 kW K⁻¹. Generation grows faster than removal, so the operating point is unstable and runaway is possible.

3. Recommend one operational change that preserves the throughput increase but restores a stable operating margin. Quantify the required UA or coolant temperature, and state one trade-off.

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To keep the higher throughput, increase heat-transfer capacity rather than simply lowering coolant temperature. At 350 K, removing 53.3 kW with 300 K coolant needs UA ≥ 1.07 kW K⁻¹, but local stability needs UA above the generation slope, about 3.1 kW K⁻¹. So a larger jacket area or higher coolant velocity is required.

Alternatively, use staged feed or feed dilution to keep local C_A and heat release lower. Trade-off: a larger UA means more pump power and capital cost; staged feed adds control complexity and may reduce conversion per pass. Simply raising C_A0 with the existing jacket is not acceptable.