An ideal heat engine is working between a source and a sink. The temperatures are raised by 100 K each, the new efficiency of the heat engine will be
equal to η
greater than η
less than η
greater or less than η depending upon the nature of the working substances
η=T1âT2T1 ηâ²=T1+100âT2+100T1+100=T1âT2T1+100 ⴠηâ²<η