The Efficiencies of Real Engines — Question 5

Section 20-6 · Physics pages 3340–3341

Question 5 Constant-pressure heat addition changes the ideal cycle efficiency An idealized Diesel cycle has reversible adiabatic compression 1 to 2 with ratio r = V1/V2 = 16, constant-pressure heating 2 to 3 with cutoffratio ρ = V3/V2 = 2, adiabatic expansion 3 to 4 back to V1, and constant-volume cooling 4 to 1. Use constant γ = 1.40 and Cp/CV = γ. V p 1 2 3 4 Axes and labels specify the model; the sketch is schematic. (a) Derive T2/T1, T3/T2 and T4/T1, then the ratio of rejected to absorbed heat. (b) Calculate efficiency and compare with the ideal Otto formula at the same compression ratio. Explain why this is not a universal ranking of actual engine designs.
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Question 5 - Solution Constant-pressure heat addition changes the ideal cycle efficiency V p 1 2 3 4 (a) Method and calculation T2/T1 = rγ−1, T3/T2 = ρ, T4/T1 = ργ. Qc Qh = CV (T4 −T1) Cp(T3 −T2) = ργ −1 γrγ−1(ρ −1). (b) Interpretation and further calculation ηD = 1 − 21.4 −1 1.4(16.4)(2 −1) ≈.613805. ηO = 1 −16−.4 ≈.670123. The comparison fixes compression ratio, not heat input, peak temperature, peak pressure or real losses. Changing those constraints changes the engineering comparison. Physical check The cutoffratio must satisfy 1 < ρ < r for the stated expansion leg.

Question 5

Constant-pressure heat addition changes the ideal cycle efficiency

An idealized Diesel cycle has reversible adiabatic compression 1 to 2 with ratio r=V1/V2=16r=V_1/V_2=16, constant-pressure heating 2 to 3 with cutoff ratio ρ=V3/V2=2\rho=V_3/V_2=2, adiabatic expansion 3 to 4 back to V1V_1, and constant-volume cooling 4 to 1. Use constant γ=1.40\gamma=1.40 and Cp/CV=γC_p/C_V=\gamma.

Diagram shown in the original SVG worksheet.

  1. Derive T2/T1T_2/T_1, T3/T2T_3/T_2 and T4/T1T_4/T_1, then the ratio of rejected to absorbed heat.

  2. Calculate efficiency and compare with the ideal Otto formula at the same compression ratio. Explain why this is not a universal ranking of actual engine designs.

Question 5 - Solution

Constant-pressure heat addition changes the ideal cycle efficiency

Diagram shown in the original SVG worksheet.

(a) Method and calculation

T2/T1=rγ−1,T3/T2=ρ,T4/T1=ργ.T_2/T_1=r^{\gamma-1},\quad T_3/T_2=\rho,\quad T_4/T_1=\rho^\gamma.QcQh=CV(T4−T1)Cp(T3−T2)=ργ−1γrγ−1(ρ−1).\frac{Q_c}{Q_h}=\frac{C_V(T_4-T_1)}{C_p(T_3-T_2)}=\frac{\rho^\gamma-1}{\gamma r^{\gamma-1}(\rho-1)}.

(b) Interpretation and further calculation

ηD=1−21.4−11.4(16.4)(2−1)≈.613805.\eta_D=1-\frac{2^{1.4}-1}{1.4(16^{.4})(2-1)}\approx.613805.ηO=1−16−.4≈.670123.\eta_O=1-16^{-.4}\approx.670123.The comparison fixes compression ratio, not heat input, peak temperature, peak pressure or real losses. Changing those constraints changes the engineering comparison.

Physical check

The cutoff ratio must satisfy 1<ρ<r1<\rho<r for the stated expansion leg.