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Gas Turbine Systems Theory 53<br />

generator drive, etc.). Compressor performance is generally shown as<br />

pressure ratio plotted against airflow. (Note: it is more accurate to<br />

use Head instead of pressure ratio, as Head takes into account the<br />

compressibility, molecular weight, temperature, and the ratio of specific<br />

heat of air—and corrected airflow—all at constant speed). This<br />

is discussed in more detail later in this chapter.<br />

Two types of compressors are in use today—they are the axial<br />

compressor and the centrifugal compressor. The axial compressor is<br />

used primarily in medium and high horsepower applications, while the<br />

centrifugal compressor is utilized in low horsepower applications.<br />

Both the axial and centrifugal compressor are limited in their<br />

range of operation by what is commonly called stall or surge. This<br />

phenomenon occurs at certain conditions of airflow, pressure ratio,<br />

and speed (rpm), which result in the individual compressor airfoils<br />

going into stall similar to that experienced by an airplane wing at a<br />

high angle of attack. The stall margin is the area between the steady<br />

state operating line and the compressor stall line.<br />

Considering the Axial Compressor<br />

Air flowing over the moving airfoil exerts lift and drag forces<br />

approximately perpendicular and parallel to the surface of the airfoil<br />

(Figure 4-3). The resultant of these forces can be resolved into two<br />

components:<br />

1. the component parallel to the axis of the compressor represents<br />

an equal and opposite rearward force on the air—causing an<br />

increase in pressure;<br />

2. a component in the plane of rotation represents the torque required<br />

to drive the compressor.<br />

From the aerodynamic point of view there are two limiting factors<br />

to the successful operation of the compressor. They are the angle<br />

of attack of the airfoil relative to the approaching air and the speed<br />

of the airfoil relative to the approaching air (Figure 4-4). If the angle<br />

of attack is too steep, the airflow will not follow the concave surface of<br />

the airfoil. This will reduce lift and increase drag. If the angle of attack<br />

is too shallow, the airflow will separate from the concave surface<br />

of the airfoil. This also results in increased drag.

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