23-Chem-A1 Process Balances and Chemical Thermodynamics · May 2013
Question 5 of 7: Heat Duty for Real-Gas Ethylene Heating
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams — May 2013 — 04-Chem-A1 Process Balances and Chemical Thermodynamics. Three-hour, open-book exam; any non-communicating calculator permitted. Format: seven questions in three parts — answer one of Q1–Q2 (Part A), one of Q3–Q4 (Part B) and two of Q5–Q7 (Part C); four questions of equal value constitute a complete paper. All seven are solved below for completeness. Where property data are needed they are stated explicitly in each Given block. Units follow the paper (mixed SI and US customary).
Reference texts: Felder, Rousseau & Bullard, Elementary Principles of Chemical Processes (4th ed., Wiley) — material & energy balances; Smith, Van Ness, Abbott & Swihart, Introduction to Chemical Engineering Thermodynamics (8th ed., McGraw-Hill) — VLE, residual properties, reaction equilibrium; supporting data from Perry's Chemical Engineers' Handbook (9th ed.) and the NIST Chemistry WebBook.
Question 5: Heat Duty for Real-Gas Ethylene Heating (equal value)
Given. Ethylene, state 1: $T_1=100\,°\text{C}=373.15$ K, $P_1=30$ bar → adiabatic (isenthalpic) valve → heat exchanger (negligible $\Delta P$) → state 2: $T_2=150\,°\text{C}=423.15$ K, $P_2=20$ bar. Ideal-gas heat capacity (A, B terms only) $C_p^{ig}/R = A+BT$ with $A=1.424$, $B=14.394\times10^{-3}\ \text{K}^{-1}$. Critical constants $T_c=282.3$ K, $P_c=50.4$ bar, $\omega=0.087$.
Find. The heat added per mole of ethylene in the exchanger, $Q$ (no flow rate is given, so on a molar basis).
Figure 5 — Adiabatic valve (state 1 → 1′, $H_{1'}=H_1$) followed by the heat exchanger (1′ → 2). Because the valve is isenthalpic, the exchanger duty is simply $Q=H_2-H_1$.
Approach. The insulated valve is isenthalpic, so the exchanger duty equals $H_2-H_1$ between the given end states; evaluate that with an ideal-gas $C_p$ term plus generalized second-virial residual enthalpies at each state.
Key simplification — the valve is isenthalpic. An adiabatic throttle does no work and adds no heat, so $H_{1'}=H_1$. The exchanger energy balance (no shaft work) is $Q=H_2-H_{1'}=H_2-H_1$: the intermediate valve-outlet temperature cancels and we only need the two given end states.
Ideal-gas enthalpy change. Using $C_p^{ig}=R(A+BT)$ from $T_1$ to $T_2$:
$$\Delta H^{ig}=R\!\left[A(T_2-T_1)+\tfrac{B}{2}(T_2^2-T_1^2)\right]=8.314\big[1.424(50)+7.197\times10^{-3}(423.15^2-373.15^2)\big]=2974\ \tfrac{\text{J}}{\text{mol}}.$$
Residual enthalpies (generalized second virial). With $H^R/(RT_c)=P_r\big[B^0-T_r\tfrac{dB^0}{dT_r}+\omega(B^1-T_r\tfrac{dB^1}{dT_r})\big]$, $B^0=0.083-0.422/T_r^{1.6}$, $B^1=0.139-0.172/T_r^{4.2}$:
$$\text{State 1 }(T_r=1.322,P_r=0.595):\ H_1^R=-882\ \tfrac{\text{J}}{\text{mol}};\qquad \text{State 2 }(T_r=1.499,P_r=0.397):\ H_2^R=-459\ \tfrac{\text{J}}{\text{mol}}.$$
Both are negative (attractive forces lower the real-gas enthalpy), and the higher-temperature, lower-pressure state 2 is closer to ideal.
Assemble the duty. Since $H=H^{ig}+H^R$,
$$Q=H_2-H_1=\Delta H^{ig}+\big(H_2^R-H_1^R\big)=2974+\big(-459-(-882)\big)=2974+423.$$
$$\boxed{Q \approx +3.40\ \text{kJ per mol of ethylene (heat added)}.}$$
The positive sign confirms heat is added; the residual correction adds ~14% to the ideal-gas estimate.
Quantity
Value
$\Delta H^{ig}$ (ideal-gas, A,B terms)
$+2974$ J/mol
$H_1^R,\ H_2^R$ (residuals)
$-882,\ -459$ J/mol
Heat added in exchanger, $Q=H_2-H_1$
$+3.40$ kJ/mol
Check: residuals use the generalized second-virial (Pitzer) correlation, valid because both states satisfy $T_r\gtrsim1.3$ and moderate $P_r$; a Lee–Kesler tabulation would agree to within a few J/mol. With no molar flow rate specified, the "rate of heat addition" is reported per mole; multiply by the molar flow to get watts.