Informazioni sul documento
- Università
- Politecnico di Milano
- Corso di laurea
- Energy Engineering
- Materia
- Fundamentals of Chemical Processes
- Classificazione
- Appunti · Completi
- Formato originale
- Testo
- Testo ricercabile
Completi di Fundamentals of Chemical Processes per il corso di Energy Engineering presso Politecnico di Milano. Materiale proveniente dall’archivio storico Studwiz e classificato per la consultazione online.
Completi di Fundamentals of Chemical Processes per il corso di Energy Engineering presso Politecnico di Milano. Materiale proveniente dall’archivio storico Studwiz e classificato per la consultazione online.
Qualità dell’importazione: il testo è stato estratto direttamente dal documento originale.
Passaggi rappresentativi riconosciuti nelle diverse parti del materiale. Il testo completo resta presente nella pagina per la ricerca, mentre l’anteprima compatta rende più semplice la lettura.
Fundamentals of Chemical Processes summary L. Spinelli 1 Chemical equilibrium In order to study chemical reactions, we must first introduce some fundamental quantities. The centrepiece of chemistry is the stoichiometry of reaction, which we can express as follows: 4NH3 + 4NO + O2 → 4N2 + 6H2O (1.1) representing the standard SCR reaction, utilised in NOx abatement. In general we can write νAA +νBB⇌νP P +νQQ (1.2) where stoichiometric coefficients νi represent how many moles of a given species are consumed/produced per unit extent of reactionε = dnA/νA = dnB/νB = dnP/νP = dnQ/νQ = dni/νi. By convention, we consider positiveνi for products, and negative for reactants. We can also introduce some important quantities such as: • conversion of species A χA = nA,converted nA,fed = n◦ A −nA n◦ A (1.3) • selectivity of A to product P SP,A = nP,produced/|νP| nA,converted/|νA| = nP −n◦ P n◦ A −nA |νA| |νP | (1.4) • yield of P from A ηP,A = nP,produced/|νP| nA,fed/|νA| = nP −n◦ P n◦ A |νA| |νP | =χA ·SP,A (1.5) 1.1 Equilibrium criteria Let’s now consider a closed system containing an arbitrary number of species, which is in equilibrium with its surroundings, that is T =Tsurr andp =psurr. The II law of thermodynamics states that dS +dSsurr ≥ 0 (1.6) where the equality holds for reversible transformations between equilibrium states: in such an instance, we havedSsurr = δQsurr Tsurr = −δQ T ⇒dS ≥ δQ T : we can plug this result into the I law of thermodynamics to write dU =δQ −pdV ⇒dU −TdS +pdV ≤ 0 (1.7) which we can further elaborate to get d (U +PV −TS )p,T =dU +pdV +Vdp −TdS −SdT ≤ 0 dG|p,T ≤ 0 (1.8) we can interpret this result as follows: any spontaneous transformation will decrease its Gibbs free energy until equilibrium is reached when dG|p,T = 0. 1 ConsideringG =G (T,p,n i)…
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