Piston pump

The two main types of piston pump are the lift pump and the force pump.^[4] Both types may be operated either by hand or by an engine.

 

 

In a lift pump, the upstroke of the piston draws water, through a valve, into the lower part of the cylinder. On the downstroke, water passes through valves set in the piston into the upper part of the cylinder. On the next upstroke, water is discharged from the upper part of the cylinder via a spout. This type of pump is limited by the height of water that can be supported by air pressure against a vacuum.

In a force pump, the upstroke of the piston draws water, through an inlet valve, into the cylinder. On the downstroke, the water is discharged, through an outlet valve, into the outlet pipe.

Piston pumps may be classified as either single-acting and single-effect (the fluid is pumped by a single face of the piston, and the active stroke is in only one direction) or double-acting and double-effect (the fluid is pumped by both faces of the piston, and the strokes in both directions are active).

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  An animation of a single-acting piston force pump.
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  An animation of a double-acting piston force pump with accumulators on both the inlet and outlet.

The calculation of a piston pump's theoretical delivery rate is relatively simple.

In a single acting pump, only one side of the piston is in contact with the fluid. As a result of this, only one stroke is a delivery stroke. The theoretical delivery rate can be calculated by using the following equation:^[5]

${\displaystyle Q=h\times {\frac {d^{2}\times \pi }{4}}\times n}$ 

Where Q is the delivery rate, d is the diameter of the piston, h is the stroke, and n is the rpm. If the pump has multiple cylinders, Q is multiplied by the number of cylinders.

In a double acting pump, both sides of the piston are in contact with the fluid. As a result of this, both strokes are delivery strokes. An approximation of the delivery rate is given by the following equation:^[5]

${\displaystyle Q=h\times {\frac {d^{2}\times \pi }{4}}\times 2n}$ 

However, this equation fails to take into consideration the volume taken up by the piston rod. The true delivery rate can be calculated accordingly:

${\displaystyle Q=nh\times \left(2{\frac {d^{2}\times \pi }{4}}-{\frac {d_{1}^{2}\times \pi }{4}}\right)=nh\times {\frac {\pi }{4}}\left(2d^{2}-d_{1}^{2}\right)}$ 

 

d₁ is equal to the diameter of the piston rod.

The piston in a plunger and piston pump does not move at a constant velocity and as a result of this the pressure and delivery fluctuate over the duration of the stroke. The following diagram shows the relation between the angle of the crankshaft and the delivery rate of a single-acting and double-acting pump. The line shows the average delivery rate of the pump. These fluctuations in pressure and delivery can cause undesired effects such as water hammer and thus are generally mitigated by the installation of an air-filled accumulator. The delivery can be further smoothed out by the use of multiple cylinders that are offset from one another.

As a result the actual delivery rate is often smaller and can be found by the following equation:

${\displaystyle Q_{s}=Q\times \lambda }$ 

Q_s is the actual delivery rate, Q is the theoretical rate, and λ is the loss coefficient.

• Axial piston pump
• Radial piston pump

• Plunger pump
• Diaphragm pump