Answer:
a) w_cycle = 721.16 KJ/kg
b) n = 0.515
c) mep = 949.2 KPa
d) T_3 = 2231.3 K
Step-by-step explanation:
Given:
-State 1: T_1 = 300K , P_1 = 1 bar
- Heat added in q_in = 1400 KJ/kg
- compression ratio r = 8.5
Find:
a) The net work, in kJ per kg of air.
b) The thermal efficiency of the cycle.
c) The mean effective pressure, in kPa
d) The maximum temperature in the cycle, in K
Solution:
Assumptions:
1) The air in the piston-cylinder is the closed system.
2) The compression and expansion processes are adiabatic, ΔP = 0.
3) All processes are internally reversible
4) The air is modeled as an ideal gas
5) Kinetic and potential energy effects are negligible
State 1:
T_1 = 300 K , P_1 = 1 bar = 100 KPa
From Air property tables:
u_1 = 214.07 kJ/ kg, V_r,1 = 621.2 m^3 / kg
State 2:
For isentropic compression
V_r,2 = V_r,1 * (V_2 / V_1) = 621.2 / 8.5 = 73.082 m^3 / kg
Hence,
T_2 = 688.2 K, u_2 = 503.06 kJ/ kg
State 3:
The specific internal energy u_3 is found by using the energy balance for process 2-3.
m * (u_3 - u_2) = Q_in
u_3 = (Q_in / m) + u_2
u_3 = q_in + u_2
u_3 = 1400 + 503.06 = 1903.6 KJ/kg
Hence,
T_3 = 2231.3 K, V_r,3 = 1.9192 m^3 / kg
State 4:
For the isentropic expansion
:
V_r,4 = V_r,3 * (V_4 / V_3 ) = V_r,3 * (V_1 / V_2 ) = 1.9192*8.5 = 16.3132 m^3 / kg
Hence,
T_4 = 1154.3 K , u_4 = 892.91 KJ/kg
part a
To find net work done of cycle w_cycle:
w_cycle = q_cycle = q_in + (u_1 - u_4)
w_cycle = 1400 + (214.07 - 892.91)
w_cycle = 721.16 KJ/kg
part b
The thermal efficiency is
:
n = w_cycle / q_in = 721.16 / 1400 = 0.515
part c
The displacement volume is V_1 - V_2 = m(v_1 - v_2 ), so the mean effective pressure is given by:
mep = w_cycle / (v_1 - v_2) = w_cycle *v_1/ (1 - 1/r)
Evaluate v_1, use ideal gas law:
v_1 = R*T_1 / P_1 = 0.2869*300/100 = 0.861 m^3/kg
mep = w_cycle *v_1/ (1 - r) = 721.16 * 0.861 / (1 - 1/8.5) = 949.2 KPa
part d
the maximum temperature of the cycle, in K
From state point 3 , we got T_3 = 2231.3 K