Pumps, Turbines, and Measurement of Flow
Pumps
Pumps are mechanical devices used to move fluids (liquids or gases) by mechanical action. They add energy to the fluid, typically in the form of pressure, to overcome resistance or lift the fluid to a higher elevation. The selection of a pump depends on factors like the fluid properties, required flow rate, head (pressure), efficiency, and cost.
Types of Pumps
Pumps are broadly classified into two main categories:
- Centrifugal Pumps
- Positive Displacement Pumps
Centrifugal Pumps
Centrifugal pumps operate by converting rotational kinetic energy into the hydrodynamic energy of the fluid flow. A rotating impeller imparts velocity to the fluid, which is then converted into pressure energy as the fluid moves through the volute casing or diffuser. They are widely used due to their simple design, relatively low cost, and ability to handle a wide range of flow rates.
Working Principle:
The fluid enters the pump casing at the eye of the impeller. As the impeller rotates, it draws the fluid into its vanes and, due to centrifugal force, throws it outwards. This increases the velocity and pressure of the fluid. The volute casing or diffuser then slows down the fluid, further increasing its pressure, before it exits the pump.
Components:
Key components include:
- Impeller: The rotating part with vanes that imparts energy to the fluid.
- Casing (Volute or Diffuser): A stationary housing that collects the fluid from the impeller and converts velocity head to pressure head.
- Shaft: Connects the impeller to the motor.
- Bearings: Support the shaft.
- Seals: Prevent leakage along the shaft.
Types of Centrifugal Pumps based on Impeller Design:
- Radial Flow: Fluid flows radially outwards. Suitable for high head, low flow.
- Axial Flow: Fluid flows parallel to the shaft. Suitable for low head, high flow (like propeller pumps).
- Mixed Flow: Combines radial and axial flow characteristics.
Characteristics:
The performance of a centrifugal pump is described by its Head-Flow (H-Q) curve, which shows the relationship between the head the pump can deliver and the flow rate. Other important curves include Power-Flow (P-Q) and Efficiency-Flow (η-Q).
Positive Displacement Pumps
Positive displacement pumps trap a fixed volume of fluid and force it into the discharge pipe. They deliver a constant flow rate regardless of the discharge pressure (within the pump's limits). They are suitable for high-viscosity fluids, high-pressure applications, and precise metering.
Types of Positive Displacement Pumps:
- Reciprocating Pumps: Use a piston or plunger moving back and forth in a cylinder. Examples include piston pumps and plunger pumps.
- Rotary Pumps: Use rotating elements like gears, lobes, or screws to trap and move the fluid. Examples include gear pumps, vane pumps, and screw pumps.
Working Principle (e.g., Gear Pump):
Two meshing gears rotate within a casing. As the gears rotate, they trap fluid in the spaces between the gear teeth and the casing. The fluid is carried around the periphery of the gears and discharged on the other side.
Characteristics:
Positive displacement pumps have a relatively flat Q-H curve, meaning the flow rate is less sensitive to changes in head. They are often self-priming and can handle high viscosities. However, they can generate very high pressures, so a relief valve is usually necessary to prevent damage if the discharge line is blocked.
Pump Performance and Selection
When selecting a pump, several factors are considered:
- Fluid Properties: Viscosity, density, temperature, corrosiveness, presence of solids.
- System Requirements: Required flow rate (Q) and total head (H). The total head includes static head (elevation difference), friction head (losses in pipes and fittings), and pressure head.
- Efficiency: Higher efficiency means lower energy consumption.
- Net Positive Suction Head (NPSH): This is a critical parameter to prevent cavitation. NPSH available (NPSHa) from the system must be greater than the NPSH required (NPSHr) by the pump.
- NPSHa = (Absolute pressure at suction flange) - (Vapor pressure of liquid) - (Friction loss in suction line)
- NPSHr is a characteristic of the pump, provided by the manufacturer.
Pump Laws (Affinity Laws)
These laws describe how the performance of a centrifugal pump changes when its speed or impeller diameter is altered. They are useful for predicting performance under different operating conditions.
| Parameter | Relationship with Speed (N) | Relationship with Impeller Diameter (D) |
|---|---|---|
| Flow Rate (Q) | Q ∝ N | Q ∝ D |
| Head (H) | H ∝ N2 | H ∝ D2 |
| Power (P) | P ∝ N3 | P ∝ D3 |
Turbines
Turbines are rotating machines that convert the energy of a moving fluid (like water, steam, or gas) into mechanical energy, which is then typically used to generate electricity. In the context of hydraulics, we primarily focus on water turbines.
Types of Water Turbines
Water turbines are classified based on the type of energy they utilize and the direction of fluid flow.
- Impulse Turbines: Utilize the kinetic energy of a high-velocity jet of water. The pressure of the water remains atmospheric throughout its passage through the turbine.
- Reaction Turbines: Utilize both the kinetic energy and the pressure energy of the water. The water pressure changes as it flows through the turbine.
Impulse Turbines
These turbines are best suited for high head and low flow conditions.
Pelton Turbine:
The Pelton turbine is the most common type of impulse turbine. It consists of a wheel with buckets mounted on its periphery. A nozzle directs a high-velocity jet of water onto these buckets, causing the wheel to rotate. The buckets are designed with a splitter ridge to divide the jet and deflect it outwards, maximizing impulse transfer.
- Head Range: Typically used for heads above 300 meters.
- Key Features: Nozzle, spear (for flow regulation), runner with buckets, casing.
- Working Principle: The high-speed jet strikes the buckets, transferring its momentum and causing rotation.
Reaction Turbines
These turbines are suitable for medium to low head and high flow conditions. They operate under pressure.
Francis Turbine:
The Francis turbine is a versatile reaction turbine, suitable for a wide range of heads (medium range). Water enters radially and exits axially. It has spiral casing (scroll case), stay vanes, guide vanes (which control flow and direct water onto the runner), and a runner with curved vanes.
- Head Range: Typically 40 to 600 meters.
- Working Principle: Water enters the scroll case, flows through the guide vanes, and strikes the curved runner blades, causing rotation. The water pressure decreases as it passes through the runner, and it exits axially through a draft tube.
Kaplan Turbine:
The Kaplan turbine is a type of axial flow reaction turbine, best suited for very low heads and high flow rates. It is similar to a propeller, with adjustable blades.
- Head Range: Typically less than 70 meters.
- Working Principle: Water flows axially through the runner, causing it to rotate. The adjustable blades allow for high efficiency even when the flow rate varies significantly.
- Components: Scroll case, guide vanes, runner with adjustable blades, draft tube.
Turbine Efficiency
The efficiency of a turbine is the ratio of the mechanical power output to the water power input. Major losses include hydraulic losses (friction, turbulence), mechanical losses (friction in bearings), and volumetric losses (leakage).
Specific Speed (Ns)
Specific speed is a dimensionless parameter used to classify turbines. It represents the speed of a geometrically similar turbine that would produce unit power when operating under unit head. It helps in selecting the appropriate type of turbine for a given head and flow condition.
The formula for specific speed is:
Ns = (N * √P) / H5/4
Where:
- N = Speed of the turbine in RPM
- P = Power output in kW
- H = Head in meters
- Low Ns: Pelton Turbine
- Medium Ns: Francis Turbine
- High Ns: Kaplan Turbine
Measurement of Flow
Accurate measurement of fluid flow rate is crucial in many engineering applications, including irrigation, water supply, industrial processes, and research. Various devices, known as flow meters or flow measurement devices, are used for this purpose.
Methods of Flow Measurement
Flow measurement can be categorized into different types based on the principle of operation.
Common Flow Measurement Devices
1. Orifice Meter
An orifice meter consists of a thin plate with a precisely drilled hole (orifice) inserted into a pipe. When fluid flows through the orifice, it causes a constriction, leading to a drop in pressure. The flow rate is determined by measuring the pressure difference across the orifice.
- Principle: Bernoulli's equation and the concept of vena contracta (the point of maximum contraction of the fluid stream).
- Formula: Q = Cd * A2 * √(2 * g * (h1 - h2) / (1 - (β)4))
- Where:
- Q = Flow rate
- Cd = Coefficient of discharge (typically 0.6 to 0.65 for sharp-edged orifices)
- A2 = Area of the orifice
- g = Acceleration due to gravity
- h1, h2 = Heads at upstream and downstream of the orifice
- β = Ratio of orifice diameter to pipe diameter (d/D)
2. Venturi Meter
A Venturi meter is a smooth constriction in a pipe with a converging section, a throat, and a diverging section. It is based on Bernoulli's principle. The converging section accelerates the fluid, and the diverging section (with a gradual angle) helps to recover most of the pressure energy, resulting in a lower permanent pressure loss compared to an orifice meter.
- Principle: Bernoulli's equation.
- Formula: Q = Cd * A1 * A2 * √(2 * g * (h1 - h2) / (A12 - A22))
- Where:
- A1 = Area of the upstream pipe
- A2 = Area of the throat
- Cd = Coefficient of discharge (typically 0.95 to 0.98)
3. Flow Nozzle
A flow nozzle is similar to an orifice but has a rounded inlet and a shorter length. It provides a better discharge coefficient and lower head loss than an orifice plate but higher head loss than a Venturi meter.
4. Pitot Tube
A Pitot tube is used to measure the local velocity of a fluid at a point. It consists of a tube inserted into the flow such that one opening faces the flow directly (stagnation point) and others are at right angles to the flow.
- Principle: Bernoulli's equation.
- Stagnation Pressure (Ps): Pressure at the point where the fluid velocity is zero.
- Static Pressure (Pstatic): Pressure of the undisturbed fluid.
- Dynamic Pressure: Ps - Pstatic = 0.5 * ρ * v2
- Velocity (v): v = √(2 * (Ps - Pstatic) / ρ)
- Where:
- ρ = Density of the fluid
To measure the average flow rate in a pipe, multiple Pitot tube readings are taken across the pipe's cross-section and averaged.
5. Weirs
Weirs are obstructions placed across an open channel (like a canal or river) over which the fluid flows. They are used to measure flow rate in open channels. The flow rate is determined by measuring the head (depth of water) above the crest of the weir.
Types of Weirs:
- Rectangular Weir: Simple rectangular notch.
- Triangular (V-notch) Weir: Notch in the shape of a V. Preferred for measuring low flow rates as it provides a larger head variation for a given flow change.
- Cipolletti Weir: A trapezoidal weir with suppressed contractions.
Formulas (Simplified):
- Rectangular Weir: Q = (2/3) * Cd * L * √(2g) * H3/2
- Triangular Weir: Q = (8/15) * Cd * tan(θ/2) * √(2g) * H5/2
- Where:
- L = Length of the weir crest
- H = Head over the weir crest
- θ = Angle of the V-notch
- Cd = Coefficient of discharge
6. Flumes
Flumes are specially shaped structures installed in open channels that constrict the flow, causing a rise in the water level upstream. By measuring this water level (head), the flow rate can be calculated. Examples include Parshall flumes. They offer less obstruction and lower head loss than weirs.
7. Electromagnetic Flow Meters
These meters measure flow rate based on Faraday's law of electromagnetic induction. A magnetic field is applied across the fluid pipe. As a conductive fluid flows through the field, it generates a voltage proportional to its velocity. These are suitable for clean liquids and slurries.
8. Ultrasonic Flow Meters
These meters use ultrasonic transducers to measure fluid velocity. They can be clamped onto the outside of the pipe (non-intrusive). They work by measuring the time difference for ultrasonic pulses traveling with and against the flow (transit-time method) or by measuring the frequency shift of reflected pulses (Doppler method).
9. Turbine Flow Meters
A small turbine or propeller is placed in the flow path. The fluid causes the turbine to rotate, and its speed is proportional to the flow rate. These are typically used for clean liquids and gases.
| Device | Principle | Application | Pressure Loss |
|---|---|---|---|
| Orifice Meter | Bernoulli's Eq. (Venturi Effect) | Pipes (general) | High |
| Venturi Meter | Bernoulli's Eq. | Pipes (accurate, low loss) | Low |
| Pitot Tube | Bernoulli's Eq. | Local velocity in pipes/aerodynamics | N/A (measures point velocity) |
| Weir | Hydraulics (open channel) | Open channels (low head) | N/A (obstructs flow) |
| Electromagnetic Flow Meter | Faraday's Law | Conductive liquids | None |
| Ultrasonic Flow Meter | Acoustics | Various liquids/gases (non-intrusive) | None |