Repeat Example 91 (gas compressed in a cylinder by a piston), but without using the continuity equation.

Question:

Repeat Example 9–1 (gas compressed in a cylinder by a piston), but without using the continuity equation. Instead, consider the fundamental definition of density as mass divided by volume. Verify that Eq. 5 of Example 9–1 is correct.


Data from Example 1

An air–fuel mixture is compressed by a piston in a cylinder of an internal combustion engine (Fig. 9–7). The origin of coordinate y is at the top of the cylinder, and y points straight down as shown. The piston is assumed to move up at constant speed VP. The distance L between the top of the cylinder and the piston decreases with time according to the linear approximation L = Lbottom – VPt, where Lbottom is the location of the piston when it is at the bottom of its cycle at time t = 0, as sketched in Fig. 9–7. At t = 0, the density of the air–fuel mixture in the cylinder is everywhere equal to ρ(0). Estimate the density of the air–fuel mixture as a function of time and the given parameters during the piston’s up stroke.


Equation 5

FIGURE 9–7

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