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Axial & Radial Thrusts 1 AXIAL THRUST 

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Axial & Radial Thrusts 

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AXIAL 

THRUST 

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AXIAL THRUST 

Axial Thrust in Single-Stage Pumps with Closed Impellers 

. Pressures generated by a Centrifugal Pump exert Forces on both Stationary and Rotating Parts.

The Design of these Parts balances Some of these Forces, butSeparate Means may be required to Counter balance Others.

. Axial Hydraulic Thrust on an impeller isthe Sum of  the Unbalanced Forces acting in Axial Direction.

. As Reliable Large-Capacity

Thrust Bearings are Now Available 

Axial Thrust in Single-Stage Pumps remains a ProblemOnly in Larger Units 

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Theoretically, a Double-Suction Impeller is in Axial Balance,with the Pressures on One Side Equal to and Counter balancing 

the Pressures on the Other (

Fig. 37). 

Fig.37 Origin of  Pressure acting on Impeller  Shrouds to produce Axial Thrust 

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In Practice, this Balance may Not be achieved for the Following:

1- The Suction Passages to the 2 Suction Eyes may not provide Equal or Uniform Flows to the 2 Sides.

2- External Conditions, such as an Elbow located too close tothe pump suction nozzle, may cause unequal flow to the twosuction eyes.

3- 2 Sides of Discharge Casing waterways may Not Symmetrical,or the Impeller may be located Off -Center .

These Conditions Causing Unequal Pressures on Shrouds.

4- Unequal Leakage through 2 Leakage joints can Upset Balance 

Combined, these Factors can create Axial Unbalance.

To Compensate for this, All Centrifugal Pumps, even thosewith Double-Suction Impellers, incorporate 

Thrust Bearings.

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Fig. 38 Pressure Distribution on:Front and Back Shrouds of Single-Suction Impeller 

With Shaft through Impeller Eye 

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To eliminate the axial thrust of a single-suction impeller, apump can be provided with both front and back wearing rings.

To equalize thrust areas, the inner diameter of both rings ismade the same (Fig. 39).

Pressure approximately equal to the suction pressure ismaintained in a chamber located on the impeller side of the backwearing ring by drilling balancing holes through the impeller.

Leakage past the back wearing ring is returned to the suctionarea through these holes.

However, with large single-stage single-suction pumps,balancing holes are considered undesirable 

because leakage

back to the impeller suction opposes the main flow, creatingdisturbances.

In such pumps, a piped  connection to the pump suction replaces the balancing holes.

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Fig. 39 Balancing Axial Thrust of  Single-Suction Impeller by means of  Wearing Ring on Back Side and Balancing Holes 

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Another way to eliminate or reduce axial thrust in single-suction impellers is touse pump-out vanes on the back shroud.

The effect of these vanes is to reduce the pressure acting on the back shroud of the impeller (Fig. 40).

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Fig. 40 Pump-out Vanes used in a Single-Suction Impeller  to reduce Axial Thrust 

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 Axial forces acting on an overhung impeller with a single stuffingbox (Fig 41) are definitely affected by suction pressure.

In addition to unbalanced force found in single-suction (Fig. 38),here is an axial force equivalent toproduct of the shaft area through the stuffing box and

The difference between suction and atmospheric pressure

This force acts: toward the impeller suction when the suction pressure is lessthan atmosphericOr  

in the opposite direction when it is higher than atmospheric.

When an overhung impeller pump handles a suction lift,The additional axial force is very low.

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Fig. 41 Axial Thrust Problem with Single-SuctionOver hung Impeller and Single Stuffing Box 

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Axial Thrust in Multistage Pumps

Most multistage pumps are built with single-suction impellers in order to simplify

the design of the inter-stage connections.

Two obvious arrangements are possible for the single-suction impellers:

1- Several single-suction impellers may be mounted on one shaft, each having itssuction inlet facing in the same direction and its stages following one another inascending order of pressure (Fig. 42).

The axial thrust is then balanced by a hydraulic balancing device.

2- An even number of single-suction impellers may be used, one-half facing in onedirection and the other half  facing in the opposite direction.

With this arrangement, axial thrust on the first half is compensated by the thrust inthe opposite direction on the other half (Fig. 43).

This mounting of single-suction impellers back to back is frequently called opposed  impel lers  . 

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Fig. 42 Multistage Pump with Single-Suction Impellersfacing in One Direction and Hydraulic Balancing Device. 

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Fig.43 4-Stage Pump with Opposed Impellers

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It is important to note that the opposed impeller arrangement  completelybalances axial thrust only under the following conditions:

1. The pump must be provided with two stuffing boxes.

2. The shaft must have a constant diameter .

3. The impeller hubs must not extend through the inter-stage portion of the casingseparating adjacent stages.

Except for some special pumps that have an internal and enclosed bearing at oneend, and therefore only one stuffing box, most multistage pumps fulfill the firstcondition.

Because of  structural requirements, however, the last two conditions are notpractical.

 A slight residual thrust is usually present in multistage opposed impeller pumps

and is carried on the thrust bearing.

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HYDRAULIC BALANCING DEVICES 

If all the single-suction impellers of a multistage pump  face in the same

direction, the total theoretical hydraulic axial thrust acting toward the suction end of the pump will be the sum of the individual impeller thrusts.

The thrust magnitude will be approximately equal to the product of the net pumppressure and the annular unbalanced area.

Actually the axial thrust is about 70 to 80% of this theoretical value.

Some form of  hydraulic balancing device must be used to balance this axialthrust and to reduce the pressure on the stuffing box adjacent to the last-stageimpeller .

This hydraulic balancing device may be: A balancing drum,

 A balancing disk, a combination of the two.

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Balancing Drums (Fig. 44)The balancing chamber at the back of the last stage impeller  is separated from

the pump interior by a drum that is either  keyed or screwed to the shaft androtates with it. 

The drum is separated by a small radial clearance from the stationary portion of the balancing device, called the balancing-drum  head , which is fixed to the pumpcasing.

The balancing chamber is connected either to:The pump suction The vessel from which the pump takes its suction

The back pressure in the balancing chamber  is only slightly higher than thesuction pressure, the difference between the two being equal to the friction losses between this chamber and the point of return.

The leakage between the drum and the drum head is a function of the differentialpressure across the drum and of the clearance area.

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Fig.44 Balancing Drum 

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The forces acting on the balancing drum in Fig. 44 are the following:

1.Toward the Discharge end:The discharge pressure multiplied by the front

balancing area (area B) of the drum.

2.Toward the Suction end:The back pressure in the balancing chamber multipliedby the back balancing area (area C) of the drum.

The first force is greater than the second, thereby counterbalancing the axialthrust exerted upon the single-suction impellers.

The drum diameter can be selected to balance axial thrust completely or within 90to 95%, depending on the desirability of carrying any thrust-bearing loads.

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Fig.45 Simple Balancing Disk 

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The inner and outer disk diameters are chosen so that the difference between thetotal force acting on the disk face and that acting on its back will balance the impeller axial thrust.

To assure proper balancing disk operation, the change in back pressure in thebalancing chamber must be of an appreciable magnitude.

This can be accomplished by  introducing a restricting orifice  in the leakagereturn line that increases back pressure when leakage past the disk increasesbeyond normal.

The disadvantage of this arrangement is that the pressure on the stuffing boxpacking is variable a condition that is injurious to the life of the packing andtherefore to be avoided.

The higher pressure that can occur at the packing is also undesirable.

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Combination Balancing Disk and Drum The combination balancing disk and drum (Fig. 46) was developed:To obviate the shortcomings of the disk while 

Retaining the advantage of automatic compensation for axial thrust changes 

In this design, radial clearance remains constant  regardless of disk position,whereas the axial clearance varies with the pump rotor position.

The following forces act on this device:

1. Toward the discharge end: the sum of the discharge pressure multiplied by area A, plus the average intermediate pressure multiplied by area B.

2. Toward the suction end: the back pressure multiplied by area C.

Here is how it works: When the pump rotor moves toward the suction end (to theleft in Fig. 46) because of increased axial thrust, the axial clearance is reduced and

pressure builds up in the intermediate relief chamber, increasing the average value of the intermediate pressure acting on area B.

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Fig.46 Combination Balancing Disk and Drum 

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There are now in use numerous Hydraulic Balancing Device Modifications.

One Typical Design separates the drum portion of a combination device into twohalves, one preceding and the second following the disk (Fig. 47).

FIG. 47 Combination Balancing Disk and Drum With Disk Located in Center Portion of Drum 

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Radial

Thrust 

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Radial Thrust In a single-volute     pump  casing  design (Fig. 4), uniform or near uniform

pressures act on the impeller when the pump is operated at design capacity. 

At other capacities, the pressures around the impeller are not uniform (Fig. 5)and there is a resultant radial reaction (F). 

Radial thrust increases as capacity decreases from that at the design flow.

Radial reaction is a function of : Total head The width and diameter of the impeller  

Thus a high-head pump with a large impeller  diameter will have a much greater radial reaction force at partial capacities than a low-head pump with a smallimpeller diameter .

The minimum reaction occurs at design capacity.

For the diffuser-type pump, the individual reactions cancel each other .

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Fig. 4 Uniform Casing Pressure exists at Design Capacity,

resulting in Zero Radial Reaction. 

Fig. 5 At Reduced Capacities Uniform Pressures do Not exist 

in a single-volute casing,resulting in a radial reaction, F 

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In a centrifugal pump design, shaft diameter  as well as bearing size can beaffected by the allowable deflection as determined by:

The shaft span,

Impeller weight,Radial reaction forces,

Torque to be transmitted

For  sustained operation  at lower capacities, the pump manufacturer  wouldsupply a heavier shaft, usually at a much higher cost.

Because of the increasing application of pumps which must operate at reducedcapacities, it has become desirable to design standard units to accommodatesuch conditions.

One solution is to use heavier shafts and bearings.

Except for low-head pumps, this solution is not economical.

The only practical answer  is a casing design that develops a much smaller radialreaction force at partial capacities. 

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One of these is the doub le  -volute   casing design, also called twin-volute   or dual-  vo lu te  design.

The application of the Double-volute design principle to neutralize radial reactionforces at reduced capacity is illustrated in Fig. 6.

The double-volute design has many hidden advantages.

For example:

In large-capacity  medium- and high-head  single-stage  vertical pumps, the rib forming the second volute and separating it from the discharge waterway of the firstvolute strengthens the casing (Fig. 7). 

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Fig. 6 Transverse view of a Double-Volute Casing Pump 

A i l & R di l Th

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Fig. 7 Sectional view of a Vertical-Shaft End-Suction Pumpwith a Double-Casing

A i l & R di l Th t

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Individual stages of a Multistage pump can be made Double Volute, Fig. 8. 

The kinetic energy discharged from the impeller must be transformed into pressure energy and turned back 180 to enter the impeller of the next stage.

The double volute therefore also acts as a return channel (back view, Fig. 8).The Guide vanes used to Straighten the Flow into the Next Stage.

Fig. 8 Double Volute of a Multistage Pump: Front view (Left) and Back view (Right). 

A i l & R di l Th t

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Fig. 9 Arrangement of Multi-Stage Volute Pump for Radial-Thrust Balance