Q23 | = m cp (T3 - T2) | (für Isobare) |
= m cp (T4 - T1) | (wegen Isothermen) | |
= Q14 = - Q41 |
Q34 | = m Ri T3 ln(p3/p4) |
= m Ri T3 ln(p2/p1) |
Q12 | = m Ri T1 ln(p1/p2) |
= - m Ri T1 ln(p2/p1) |
|Wk| | = Q34 + Q12 |
= m Ri (T3 - T1) ln(p2/p1) |
ηth | = |Wk|/Q34 |
= 1 - T1/T3 |