A diesel engine works at a high compression ratio to compress air until it reaches a temperature high enough to ignite the diesel fuel. Suppose the compression ratio (ratio of volumes) of a specific diesel engine is 20 to \(1 .\) If air enters a cylinder at 1.00 atm and is compressed adiabatically, the compressed air reaches a pressure of 66.0 atm. Assuming that the air enters the engine at room temperature \(\left(25.0^{\circ} \mathrm{C}\right)\) and that the air can be treated as an ideal gas, find the temperature of the compressed air.

In thermodynamics, the adiabatic process is characterized by the absence of heat transfer between the system and its surroundings. When considering such a process in the context of diesel engines, understanding the adiabatic equation becomes crucial.

This equation, which applies to ideal gases under adiabatic compression or expansion, can be expressed as:
\[P_1 V_1^\gamma = P_2 V_2^\gamma\]
where:

• \(P_1\) and \(P_2\) are the initial and final pressures, respectively,
• \(V_1\) and \(V_2\) are the initial and final volumes,
• and \(\gamma\) is the heat capacity ratio (discussed in a later section).

In a diesel engine, the air undergoes adiabatic compression, increasing its pressure and temperature until it's hot enough to ignite diesel fuel. The adiabatic equation allows us to relate the change in volume and pressure to the change in temperature, which is vital for determining the conditions necessary for fuel combustion.

The ideal gas law is a fundamental equation in chemistry and physics that relates the pressure, volume, and temperature of an ideal gas. It's typically stated as:
\[PV = nRT\]
where:

• \(P\) is the pressure,
• \(V\) is the volume,
• \(n\) is the number of moles,
• \(R\) is the universal gas constant,
• and \(T\) is the temperature in Kelvin.

In the context of a diesel engine, the ideal gas law is used after applying the adiabatic equation to relate the pressures and volumes at two different states. As the ideal gas law assumes no interaction between gas molecules, it greatly simplifies calculations for the temperature and pressure conditions within the engine's cylinders.

The heat capacity ratio, often denoted as \(\gamma\) (gamma), is a dimensionless quantity and an essential parameter in adiabatic processes. It's defined as the ratio of the specific heat capacity at constant pressure \(C_p\) to the specific heat capacity at constant volume \(C_v\):
\[\gamma = \frac{C_p}{C_v}\]
This ratio affects how gases behave when compressed or expanded without heat exchange. For diatomic gases, such as the nitrogen and oxygen primarily found in air, \(\gamma\) is approximately 1.4.

The value of \(\gamma\) is crucial when applying the adiabatic equation, as it directly influences the final temperature and pressure of the compressed gas in the diesel engine. Knowing \(\gamma\) helps predict how efficiently the engine compresses air and, consequently, its ability to reach the temperature required for fuel ignition.

The compression ratio is a key concept in the design and function of diesel engines. It's defined as the ratio of the maximum volume in the cylinder when the piston is at the bottom of its stroke (the bottom dead center, BDC) to the minimum volume when the piston is at the top of its stroke (the top dead center, TDC):
\[\text{Compression ratio} = \frac{V_{\text{BDC}}}{V_{\text{TDC}}}\]
In diesel engines, a high compression ratio is used to compress the air so significantly that the temperature rises to a level that can ignite diesel fuel without the need for a spark plug. As demonstrated in the exercise, a compression ratio of 20 to 1 means the volume of air is reduced by a factor of 20 during the compression stroke. A higher compression ratio typically results in higher efficiency and more power output from the engine, but it also requires stronger engine components to withstand the greater pressures produced.