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An axial-flow pump, or AFP, is a common type of pump that essentially consists of a propeller (an axial impeller) in a pipe. The propeller can be driven directly by a sealed motor in the pipe or by electric motor or petrol/diesel engines mounted to the pipe from the outside or by a right-angle drive shaft that pierces the pipe. Fluid particles, in course of their flow through the pump, do not change their radial locations since the change in radius at the entry (called 'suction') and the exit (called 'discharge') of the pump is very small. Hence the name "axial" pump. Operation An axial flow pump has a propeller-type of impeller running in a casing. The pressure in an axial flow pump is developed by the flow of liquid over the blades of impeller. The fluid is pushed in a direction parallel to the shaft of the impeller, that is, fluid particles, in course of their flow through the pump, do not change their radial locations. It allows the fluid to enter the impeller axially and discharge the fluid nearly axially. The propeller of an axial flow pump is driven by a motor. Notes The fixed diffuser vanes are used to remove the whirl component ( V w 2 {\displaystyle V_{\rm {w2}}} ) of the discharge velocity of the impeller and to convert the energy to pressure. The impeller vanes may be adjustable. The machine may be fitted with pre-entry vanes to eliminate pre-rotation and to make the flow purely axial. Work done on the fluid per unit weight = U ( V w 2 − V w 1 ) g {\displaystyle U{\frac {(V_{\rm {w2}}-V_{\rm {w1}})}{g}}} where U = U 2 = U 1 {\displaystyle U=U_{\rm {2}}=U_{\rm {1}}} is the blade velocity. For maximum energy transfer, V w 1 = 0 {\displaystyle V_{\rm {w1}}=0} , that is, α 1 = 90 ∘ {\displaystyle \alpha _{\rm {1}}=90^{\circ }} Therefore, from outlet velocity triangle, we have Therefore, the maximum energy transfer per unit weight by an axial flow pump = U ( U − V f 2 cot ⁡ β 2 ) g {\displaystyle U{\frac {(U-V_{\rm {f2}}\cot \beta _{\rm {2}})}{g}}} Blade design In an axial flow pump, blades have an airfoil section over which the fluid flows and pressure is developed. For a constant flow, we have V f 1 = V f 2 = V f {\displaystyle V_{\rm {f1}}=V_{\rm {f2}}=V_{\rm {f}}} So, the maximum energy transfer to the fluid per unit weight will be For constant energy transfer over the entire span of the blade, the above equation should be constant for all values of r {\displaystyle r} . But, U 2 {\displaystyle U^{2}} will increase with an increase in radius r {\displaystyle r} , therefore to maintain a constant value an equal increase in U V f cot ⁡ β 2 {\displaystyle UV_{\rm {f}}\cot \beta _{\rm {2}}} must take place. Since, V f {\displaystyle V_{\rm {f}}} is constant, therefore cot ⁡ β 2 {\displaystyle \cot \beta _{\rm {2}}} must increase on increasing r {\displaystyle r} . So, the blade is twisted as the radius changes. Characteristics The characteristics of an axial flow pump are shown in the figure. As shown in the figure, the head at the zero flow rate can be as much as three times the head at the pump's best efficiency point. Also, the power requirement increases as the flow decreases, with the highest power drawn at the zero flow rate. This characteristic is opposite to that of a centrifugal pump where power requirement increases with an increase in the flow. Also the power requirements and pump head increases with an increase in pitch, thus allowing the pump to adjust according to the system conditions to provide the most efficient operation. Advantages The main advantage of an axial flow pump is that it has a relatively high discharge (flow rate) at a relatively low head (vertical distance). For example, it can pump up to 3 times more water and other fluids at lifts of less than 4 meters as compared to the more common radial-flow or centrifugal pump. It also can easily be adjusted to run at peak efficiency at low-flow/high-pressure and high-flow/low-pressure by changing the pitch on the propeller (some models only). The effect of turning of the fluid is not too severe in an axial pump and the length of the impeller blades is also short. This leads to lower hydrodynamic losses and higher stage efficiencies. The.... Discover the Merle C Potter popular books. Find the top 100 most popular Merle C Potter books.