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FLOW MEASUREMENT
Positive Displacement Meter
Nutatin Disc
Oval gear type
Helix type.
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Positive Displacement Flowmeter
Measures the volume of fluid passing
through the flowmeter
This achieved by repeatedly filling a bucketwith fluid before dumping the contents
downstream.
Number of times that the bucket is filled and
emptied is indicative of the flow through the
flow meter
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Nutating Disc
also known as disk meter, is used extensively
for residential water service.
The moving assembly, which separates thefluid into increments consists of an assembly
of a radially slotted disk with an integral ball
bearing and an axial pin.
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Nutating Disc
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Nutating Disc
Metering chamber divided into four volumes,
two above the disk on the inlet side and two
e ow e s on e ou e s e. Pressure drop from inlet to outlet causes the
disk to wobble or nutate,
For each cycle to display a volume equal to
the volume of the metering chamber minus
the volume of the disk assembly.
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Nutating Disc
The end of the axial pin, which moves in a
circular motion, drives a cam that is connected
o a gear ra n an e o a z ng reg s er. Inaccuracy : 1 to 2%.
Temperature range : 150 to 120C.
Max working pressure : 10 kg/cm2.
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Oval Gear Type
A special variety of the rotating tube flow
meter is the oval geared metering elements.
These oval-geared meters are generally usedon very low viscous liquid, which is difficult
to measure using other flow meters.
A precise volume of liquid is captured by the
gap formed between housing and the gear
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Oval Gear Type
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Oval Gear Type
In position A, uniform forces are applied equallyon the top and bottom of oval gear B, so that theear does not rotate.
Rotor A has entrapped a known volume of liquidbetween the rotor and the meter body, and there isa balanced force on the bottom of the gear.
However, there is a force on the bottom of gear A,causing it to rotate clockwise (CW). This causesgear B to rotate in a counter clock wise (CCW)
direction to position B.
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Oval Gear Type
In position B, fluid enters the space between
gear B and the meter body, as the fluid that was
en rappe e ween gear an e o ysimultaneously leave the area of entrapment.
The higher upstream pressure oppose the lower
downstream pressure at the ends of gear A andgear B, which makes gear A and gear B
continue to rotate in CW and CCW directions
respectively, to position C.
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Oval Gear Type
In position C, a known amount of fluid has been
entrapped between gear B and the meter body.
This operation is then repeated, with eachrevolution of the gears representing the passage
of four times the amount of fluid that fills the
space between the gear and the meter body. Therefore, the fluid flow is directly proportional
to the rotational velocity of the gears.
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Oval Gear Type
If slippage between the oval-gears and the housingis small, and the flow rate and viscosity are high,these flow meters can rovide hi h accuracies.
(0.1%). These flow meters are available in the sizes
suitable for 6 mm to 400 mm diameters pipelines.
Their materials of construction include brass,carbon steel, and 316 stainless steel.
Operating pressures are available up to 100
kg/cm2 and temperatures up to 300C.
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Helix Type Flow Meters
Utilizes two uniquely nested, radically pitched
helical rotors as the measuring elements.
Close machining tolerances ensure minimumslippage and thus high accuracy.
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Rotameter
In this meter, a weighted float or plummet
contained in an upright tapered tube, is lifted to
e pos on o equ r um e ween edownward force of the plummet and the upward
force of the fluid in addition to the buoyancy
effect of the fluid flowing past the float throughthe annular orifice.
The flow rate can be read by observing the
position of the float.
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Rotameter
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Rotameter - Theory
Consists of a tapered metering tube and a floatwhich is free to move up and down within the
.
The metering tube is mounted vertically with the
small end at the bottom.
The fluid to be measured enters at the bottom ofthe tube, passes upward around the float, and
out at the top.
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Rotameter - Theory
When there is no flow through the meter, the
float rests at the bottom of the metering tube
w ere e max mum ame er o e oa sapproximately the same as the bore of the tube.
When fluid enters the metering tube, the
buoyant effect of the fluid lightens the float, butit has a greater density than the liquid and the
buoyant effect is not sufficient to raise it.
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Rotameter - Theory
There is a small annular opening between the float andthe tube.
The pressure drop across the float increases and raises the
the upward hydraulic forces acting on it are balanced byits weight less buoyant force.
The metering float is floating in the fluid stream.
The float moves up and down in the tube in proportion tothe fluid flow rate and the annular area between the floatand the tube.
It reaches a stable position in the tube when the forces are
in equilibrium.
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Rotameter - Theory
With upward movement of the float towards thelarger end of the tapered tube, the annularopening between the tube and the float
increases. As the area increases, the pressure differential
across the float decreases.
The float assumes a position, in dynamicequilibrium, when the pressure differentialacross the float plus the buoyancy effect
balances the weight of the float.
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Rotameter - Theory
Any further increase in flow rate causes the float torise higher in the tube ; a decrease in flow causesthe float to dro at a lower osition.
Every float position corresponds to one particularflow rate and no other for a fluid of a given densityand viscosity.
It is merely necessary to provide a reading orcalibration scale on the tube and flow rate can bedetermined by direct observation of the position of
the float in the metering tube.
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Rotameter - Theory
According to Bernoullis Theorem
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Rotameter - Theory
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Rotameter - Theory