The most common car engine is a 4-cylinder 4-stroke engine. The car manufacturers have a great pressure to lower the cost of the cars and this deal also with the engines. The challenges are the coming new emission norms (for example EURO-6) and also the customer acceptance, because of the fact, that the car drives are used to the 4-cylinder engine and they want to have the same driving fun also from the new engines. A 2-cylinder 2-stroke engine has the same power output and torque as a 4-cylinder 4-stroke engine and thus it offers the same driving fun. Equal balancing is easy to make without some big additional costs, if the gas exchange of the engine is made by using poppet valves and camshafts. As there are only about 70% of the moving parts in the engine, its acceleration is even better than by a 4-cylinder engine. One of the latest development in 2-stoke engines is the Z-engine (1), having the compression partially transferred outside of the working cylinders. This offers new thermo dynamical possibilities to adjust the working cycle and the combustion. As there are methods to control the temperature at TDC, a HCCI-combustion is possible in the Z-engine at all loads. This lowers significantly the cost of the engine, as no urea injection, or NOx catalyst is needed to pass the coming EU-6 emission norm. The cost of the Z-engine is lower also because of the fact that it has only 2 working cylinders instead of 4. In 1999, Aumet Oy (73) began to research this 2-stroke car diesel engine, called the Z-engine, in co-operation with the Internal Combustion Engine Laboratory at the Helsinki University of Technology (HUT) and the Energy Technology Department at the Lappeenranta University of Technology (LUT). So far, four master’s theses, one doctor theses, five SAE Papers (71, 72) and four Fisita Papers have been completed on the subject. Modern simulation tools, such as Star CD, GT-Power, Diesel RK, Fluent and Chemkin have been used. The prototype engine made its start in December 2004 and it was tested two years in a test bench at VTT. In the HCCI combustion simulation of the Z-engine, a 4-dimensional ignition delay map, calculated with Chemkin and integrated in Diesel RK (74), has been used. The simulations and tests (1) with the test engine show that the Z-engine has a very good efficiency, especially at part load. A diesel fuel HCCI-combustion at all loads is possible in the Z-engine, with lambda about 1,5-1,7 and EGRrate 15-45%, depending of the load. The TDC-temperature at part load is about 800 K and at full load (BMEP 30 bar) about 700 K. The HCCI-ignition, triggered with a small amount of diesel fuel injection close to TDC (RCCI, based on the reactivity difference on lambda of the two air-fuel mixtures in the cylinder: early injected and ignition injection), occurs between 0°20° ATDC and this limits the pressure and maximal temperature. No knock is present, as the ignition occurs always at the right side of the NTC (negative temperature coefficient) regime (30,31). NOx values are very low as the maximal temperature at full load is about 1900 K, because of the low starting temperature of the combustion, intern EGR and the expansion during the combustion. Intern EGR and active radicals stabilize the combustion (32-37) and lower the activation energy needed for the ignition. The robust HCCI-combustion without ignition problems (forced ignition, very early diesel fuel injection and thus active radicals) has been validated with 2-stroke test engines in Dr. Zhengs Doctor Theses together with his research colleges in Drexel University, Philadelphia, USA, 2005, (36). The fuel consumption is: part load 192 g/kWh, best point 174 g/kWh and full load 188 g/kWh. The part load efficiency is much better than by PCI and dual fuel RCCI, best point and full load values are of the same order. The explanation for the very good part load efficiency is the exergy increase , when the intercooled, compressed air is led in to the work cylinder and mixed with the hot, almost atmospheric combustion gases , having high intern energy, but almost zero exergy. The pressure increase at the end of the gas exchange increases also the efficiency. This is easy to understand, when seeing the gas exchange simulations, made with CFD, Appendix 2. The very short time in the gas exchange of the Z-engine, about one millisecond, makes the need of the understanding of the gas dynamics very important. The acceleration of the gas in the intake channel, as much as 50000G and the high velocity leads to high pressure rise at the end of the gas exchange, at full load up to 10 bar ( Appendix 2). This is not the case with normal engines. This very unique combination of thermodynamic and gas dynamic, first time in the history of the combustion engines, makes it possible to start the work cycle, as already Diesel wanted: isotherm and isentropic compressions, according to Carnot (see in TS). The