A tank of plan area \(5 \mathrm{~m}^{2}\), open to atmosphere at the top, is supplied through a pipe \(50 \mathrm{~mm}\) diameter and \(40 \mathrm{~m}\) long which enters the base of the tank. A pump, providing a constant gauge pressure of \(500 \mathrm{kPa}\), feeds water to the inlet of the pipe which is at a level \(3 \mathrm{~m}\) below that of the base of the tank. Taking \(f\) for the pipe as \(0.008\), calculate the time required to increase the depth of water in the tank from \(0.2 \mathrm{~m}\) to \(2.5 \mathrm{~m}\). If the combined overall efficiency of pump and driving motor is \(52 \%\), determine (in \(\mathrm{kW} \cdot \mathrm{h})\) the total amount of electricity used in this pumping operation.

Short Answer

Expert verified
The tank takes approximately 17.42 minutes to fill. The total electricity used is about 4.69 kWh.

Step by step solution

01

Determine the flow rate through the pipe

First, calculate the cross-sectional area of the pipe using the diameter: \[ A = \pi \left( \frac{d}{2} \right)^2 \] where \(d = 50 \text{ mm} = 0.05 \text{ m}\). This gives: \[ A = \pi \left( \frac{0.05}{2} \right)^2 = 1.9635 \times 10^{-3} \text{ m}^2 \] Next, use the Darcy-Weisbach equation to find the head loss due to friction in the pipe: \[ h_f = f \cdot \frac{L}{D} \cdot \frac{v^2}{2g} \] where \(f = 0.008\), \(L = 40 \text{ m}\), \(D = 0.05 \text{ m}\), and \(v\) is the fluid velocity. Express velocity \(v\) in terms of flow rate \(Q\): \[ Q = A \cdot v \Rightarrow v = \frac{Q}{A} \] Substituting into the head loss equation and solving for \(Q\): \[ h_f = f \cdot \frac{L}{D} \cdot \frac{\left( \frac{Q}{A} \right)^2}{2g} \]
02

Calculate the total head rise

The total head rise in the system can be calculated by adding the height difference and the head loss in the pipe: \[ H_t = H_p + 3 \text{ m} + h_f \] where \(H_p\) is the head provided by the pump. Using the pump pressure: \[ H_p = \frac{P_g}{\rho g} \Rightarrow H_p = \frac{500,000 \text{ Pa}}{1000 \text{ kg/m}^3 \cdot 9.81 \text{ m/s}^2} = 50.96 \text{ m} \]
03

Solve for the flow rate \(Q\)

Combining the head rise with the head loss equation, substitute \(Q\) and solve: \[ H_t = H_p + 3 + f \cdot \frac{L}{D} \cdot \frac{\left( \frac{Q}{A} \right)^2}{2g} \] \[ 50.96 + 3 = 50.96 + 3 + 0.008 \cdot \frac{40}{0.05} \cdot \frac{\left( \frac{Q}{1.9635 \times 10^{-3}} \right)^2}{2 \cdot 9.81} \Rightarrow 53.96 = 50.96 + 0.008 \cdot 800 \cdot \frac{\left( \frac{Q}{1.9635 \times 10^{-3}} \right)^2}{2 \cdot 9.81} \]
04

Simplify and solve for flow rate

Simplify the equation to solve for \(Q\): \[ 3 = \frac{0.008 \cdot 800}{2 \cdot 9.81} \cdot \left( \frac{Q^2}{1.9635 \times 10^{-3}} \right) \] \[ Q^2 = \frac{3 \cdot 2 \cdot 9.81}{0.008 \cdot 800} \cdot (1.9635 \times 10^{-3}) \] Solving for \(Q\): \[ Q = \sqrt{\frac{3 \cdot 2 \cdot 9.81 \cdot 1.9635 \times 10^{-3}}{0.008 \cdot 800}} \approx 0.011 \text{ m}^3/\text{s} \]
05

Calculate the time required to fill the tank

Calculate the volume of water needed to raise the depth from 0.2 m to 2.5 m in the tank with a plan area of 5 m²: \[ V = A \cdot (h_{2} - h_{1}) = 5 \text{ m}^2 \cdot (2.5 \text{ m} - 0.2 \text{ m}) = 11.5 \text{ m}^3 \] The time required to fill this volume at the calculated flow rate: \[ t = \frac{V}{Q} = \frac{11.5 \text{ m}^3}{0.011 \text{ m}^3/\text{s}} = 1045.45 \text{ s} \approx 17.42 \text{ minutes} \]
06

Determine the total energy usage

Calculate the total energy used by the pump: \[ P = \rho g Q H_p \] and the total energy over the time: \[ E = P \cdot t \] Convert in terms of efficiency and kilowatt-hours: \[ E_{total} = \frac{E}{\eta} = \frac{1045.45 \text{ s} \cdot 0.011 \text{ m}^3/\text{s} \cdot 1000 \text{ kg/m}^3 \cdot 9.81 \text{ m/s}^2 \cdot 50.96 \text{ m}}{0.52 \cdot 3.6 \times 10^6} \approx 4.69 \text{ kW} \cdot \text{h} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Darcy-Weisbach equation
The Darcy-Weisbach equation is vital in fluid mechanics for estimating head loss due to friction in pipes. It is represented as: \[ h_f = f \frac{L}{D} \frac{v^2}{2g} \] where:
- \( h_f \): Head loss due to friction (m or ft)
- \( f \): Friction factor (dimensionless)
- \( L \): Length of the pipe (m or ft)
- \( D \): Diameter of the pipe (m or ft)
- \( v \): Flow velocity of the fluid (m/s or ft/s)
- \( g \): Acceleration due to gravity (9.81 m/s² or 32.2 ft/s²)
To calculate the head loss, you need the pipe's diameter, length, fluid velocity, and friction factor. The friction factor \( f \) is often determined experimentally or found using the Moody chart, depending on the Reynolds number and pipe roughness. For the problem at hand, knowing these parameters allows the calculation of head loss, which impacts the system's total head.
Pump Efficiency
Pump efficiency is a crucial metric that determines how well a pump converts electrical energy into hydraulic energy. Mathematically, it can be written as: \[ \text{Efficiency} (\boldsymbol{\text{η}}) = \frac{\text{Hydraulic Power Output}}{\text{Electrical Power Input}} \times 100% \]
For example, if a pump has an efficiency of 52%, it means that only 52% of the electrical energy is converted into useful work in lifting water, while the rest is lost to factors like heat and friction. In the exercise, calculating the efficiency of the pumping system helps determine the total energy consumption. This efficiency metric is critical for designing energy-efficient systems and estimating operational costs accurately.
Flow Rate Calculation
Flow rate is a measure of the volume of fluid passing through a cross-section of a pipe per unit time. It is usually denoted by \( Q \) and can be calculated using the formula: \[ Q = A \times v \] where:
- \( Q \): Flow rate (m³/s or ft³/s)
- \( A \): Cross-sectional area of the pipe (m² or ft²)
- \( v \): Flow velocity (m/s or ft/s)
In the given problem, calculating the flow rate requires finding the area first using the diameter of the pipe: \[ A = \frac{\boldsymbol{\text{π}}}{4} D^2 \]
Then, we use this area to find the velocity \( v \), which in turn helps determine the flow rate. Accurate flow rate calculation is indispensable for estimating the time required to fill the tank from one depth to another.
Head Loss
Head loss refers to the energy lost due to friction and other resistance factors as fluid flows through a pipe. It is a key consideration in designing piping systems and pumps. Factors contributing to head loss include pipe length, diameter, flow speed, and the fluid's viscosity.
There are two main types of head loss:
  • **Major Head Loss:** Caused by friction within the pipe's walls, primarily determined by the Darcy-Weisbach equation.
  • **Minor Head Loss:** Caused by fittings, bends, valves, and other pipeline components.

In the example, calculating head loss due to friction allows us to understand the total head rise needed. Adding this to the height difference and the pump’s head helps determine the effective energy conversion required to pump water to the desired level in the tank. Properly accounting for head loss ensures that the system operates efficiently, avoiding under or over-sizing of pumps and pipes.

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Most popular questions from this chapter

A pipe \(600 \mathrm{~mm}\) diameter and \(1 \mathrm{~km}\) long with \(f=0.008\) connects two reservoirs having a difference in water surface level of \(30 \mathrm{~m}\). Calculate the rate of flow between the reservoirs and the shear stress at the wall of the pipe. If the upstream half of the pipe is tapped by several side pipes so that one-third of the quantity of water now entering the main pipe is withdrawn uniformly over this length, calculate the new rate of discharge to the lower reservoir. Neglect all losses other than those due to pipe friction.

In a heat exchanger there are 200 tubes each \(3.65 \mathrm{~m}\) long and \(30 \mathrm{~mm}\) outside diameter and \(25 \mathrm{~mm}\) bore. They are arranged axially in a cylinder of \(750 \mathrm{~mm}\) diameter and are equally spaced from one another. A liquid of relative density \(0.9\) flows at a mean velocity of \(2.5 \mathrm{~m} \cdot \mathrm{s}^{-1}\) through the tubes and water flows at \(2.5 \mathrm{~m} \cdot \mathrm{s}^{-1}\) between the tubes in the opposite direction. For all surfaces \(f\) may be taken as \(0.01\). Neglecting entry and exit losses, calculate (a) the total power required to overcome fluid friction in the exchanger and \((b)\) the saving in power if the two liquids exchanged places but the system remained otherwise unaltered.

A hose pipe of \(75 \mathrm{~mm}\) bore and length \(450 \mathrm{~m}\) is supplied with water at \(1.4 \mathrm{MPa}\). A nozzle at the outlet end of the pipe is \(3 \mathrm{~m}\) above the level of the inlet end. If the jet from the nozzle is to reach a height of \(35 \mathrm{~m}\) calculate the maximum diameter of the nozzle assuming that \(f=0.01\) and that losses at inlet and in the nozzle are negligible. If the efficiency of the supply pump is \(70 \%\) determine the power required to drive it.

Calculate the power required to pump sulphuric acid (dynamic viscosity \(0.04 \mathrm{~Pa} \cdot \mathrm{s}\), relative density \(1.83\) ) at \(45 \mathrm{~L} \cdot \mathrm{s}^{-1}\) from a supply tank through a glass-lined \(150 \mathrm{~mm}\) diameter pipe, \(18 \mathrm{~m}\) long, into a storage tank. The liquid level in the storage tank is \(6 \mathrm{~m}\) above that in the supply tank. For laminar flow \(f=16 / \mathrm{Re}\); for turbulent flow \(f=0.0014\left(1+100 \mathrm{Re}^{-1 / 3}\right)\) if \(\mathrm{Re}<10^{7}\). Take all losses into account.

A fluid of constant density \(\varrho\) enters a horizontal pipe of radius \(R\) with uniform velocity \(V\) and pressure \(p_{1}\). At a downstream section the pressure is \(p_{2}\) and the velocity varies with radius \(r\) according to the equation \(u=2 V\left\\{1-\left(r^{2} / R^{2}\right)\right\\}\). Show that the friction force at the pipe walls from the inlet to the section considered is given by \(\pi R^{\frac{1}{2}}\left(p_{1}-p_{2}-\varrho V^{2} / 3\right)\).

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