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Water flows at \(5.4 \mathrm{~m}^{3} \cdot \mathrm{s}^{-1}\) under a wide sluice gate into a rectangular prismatic channel \(3.5 \mathrm{~m}\) wide. A hydraulic jump is formed just downstream of a section where the depth is \(380 \mathrm{~mm}\). Calculate the depth downstream of the jump and the power dissipated in it.

Short Answer

Expert verified
The depth downstream of the jump is approximately 1.82 m. The power dissipated is approximately 75.43 kW.

Step by step solution

01

- Convert Depth to Meters

The depth of the channel given is 380 mm. Convert this value into meters: \[ 380 \text{ mm} = 0.38 \text{ m} \]
02

- Calculate Froude Number Before the Jump

The Froude number is given by: \[Fr_1 = \frac{Q}{b \cdot y_1^2 \cdot \sqrt{g \cdot y_1}}\] Where,\( Q = 5.4 \, \mathrm{m}^3 \, \mathrm{s}^{-1} \), \( b = 3.5 \, \mathrm{m} \), \( y_1 = 0.38 \, \mathrm{m} \), and \( g = 9.81 \, \mathrm{m} \, \mathrm{s}^{-2} \). Calculating the Froude number: \[Fr_1 = \frac{5.4}{3.5 \cdot 0.38^2 \cdot \sqrt{9.81 \cdot 0.38}} \approx 3.75\]
03

- Use Hydraulic Jump Formula for Depth After the Jump

The depth after the hydraulic jump, \( y_2 \), can be calculated using the following relationship: \[ y_2 = \frac{y_1}{2} \left(\sqrt{1 + 8 \cdot Fr_1^2} - 1\right) \] Substitute \( y_1 = 0.38 \mathrm{~m} \) and \( Fr_1 \approx 3.75 \): \[ y_2 = \frac{0.38}{2} \left(\sqrt{1 + 8 \cdot 3.75^2} - 1\right) \] Calculate the terms inside the square root first: \[ 1 + 8 \cdot 3.75^2 = 113.5 \] Thus, \[ y_2 = \frac{0.38}{2} \left(\sqrt{113.5} - 1\right) \approx \frac{0.38}{2} \times (10.65 - 1) \approx 1.82 \mathrm{~m} \]
04

- Calculate Power Dissipated in the Jump

The power dissipated in the hydraulic jump can be calculated using: \[ P = \rho \cdot g \cdot Q \cdot (y_2 - y_1) \] Where, \( \rho = 1000 \mathrm{~kg} \cdot \mathrm{m}^{-3} \), \( g = 9.81 \mathrm{~m} \cdot \mathrm{s}^{-2} \), \( Q = 5.4 \mathrm{~m}^3 \cdot \mathrm{s}^{-1} \), \( y_1 = 0.38 \mathrm{~m} \), \( y_2 = 1.82 \mathrm{~m} \). Substituting these values in, \[ P = 1000 \cdot 9.81 \cdot 5.4 \cdot (1.82 - 0.38) \approx 75425.04 \mathrm{~W} \approx 75.43 \mathrm{~kW} \]

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Key Concepts

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

Froude Number
The Froude number is a critical concept when studying hydraulic jumps. It is a dimensionless number used to compare the inertia of the fluid to the gravitational force acting on it. This helps in predicting flow patterns in open channels.
In our problem, we use the Froude number to understand the flow condition before the hydraulic jump. The formula to calculate it is:
\[ Fr_1 = \frac{Q}{b \times y_1^2 \times \text{sqrt}(g \times y_1)} \]
Here,
  • Q is the flow rate (in cubic meters per second),
  • b is the channel width,
  • y_1 is the initial depth,
  • g is the acceleration due to gravity.
For our exercise, with given values: \[ Q = 5.4 \text{ m}^3/\text{s}, b = 3.5 \text{ m}, y_1 = 0.38 \text{ m}, \text{and} g = 9.81 \text{ m/s}^2 \]
The Froude number before the jump is: \[ Fr_1 \text{ is approximately } 3.75 \]
A higher Froude number indicates a more turbulent state, which leads to a hydraulic jump.
Power Dissipation
Power dissipation in a hydraulic jump is the energy lost due to turbulence when the flow changes from rapid (supercritical) to slow (subcritical). This loss is significant and contributes to changes in water surface levels.
To calculate the power dissipated in our problem, we use the formula:
\[ P = \rho \times g \times Q \times (y_2 - y_1) \]
Where:
  • \( \rho \) is the density of water (typically 1000 kg/m³),
  • g is the acceleration due to gravity,
  • Q is the flow rate,
  • y_1 and y_2 are the depths before and after the jump.
Substituting our values: \[ \rho = 1000 \text{ kg/m}^3, g = 9.81 \text{ m/s}^2, Q = 5.4 \text{ m}^3/\text{s}, y_1 = 0.38 \text{ m}, \text{and} y_2 = 1.82 \text{ m} \]
The power dissipated is calculated as: \[ P \text{ is approximately } 75.43 \text{ kW} \]
This shows the immense amount of energy transformed due to the hydraulic jump.
Hydraulic Jump Depth Change
A hydraulic jump involves a sudden change in water depth as fast-flowing water slows down and becomes deeper. The relationship between the initial and final depths can be derived using the Froude number.
In our exercise, we calculate the depth after the jump (\( y_2 \)) using:\[ y_2 = \frac{y_1}{2} \times (\text{sqrt}(1 + 8 \times Fr_1^2) - 1) \]
Given: \( y_1 = 0.38 \text{ m} \text{ and } Fr_1 = 3.75 \)
First, compute the inner term: \[ 1 + 8 \times 3.75^2 = 113.5 \]
Next, find the square root: \[ \text{sqrt}(113.5) \text{ is approximately } 10.65 \]
Then subtract 1 and divide by 2: \[ \frac{10.65 - 1}{2} \text{ is approximately } 4.825 \]
Finally, multiply by the initial depth: \[ 0.38 \times 4.825 = 1.82 \text{ m} \]
Thus, the depth after the hydraulic jump is approximately 1.82 meters. This shows how the depth increases significantly due to the hydraulic jump.
Flow Rate Conversion
Flow rate conversion is an important step in hydraulic calculations. The flow rate in our problem is given in \( \text{m}^3/\text{s} \) (cubic meters per second).
Sometimes, it might be necessary to convert this to other units. To do this, consider the following:
  • 1 \( \text{m}^3/\text{s} \) = 1000 \( \text{L/s} \) (liters per second)
  • ,
  • 1 \( \text{m}^3/\text{s} \) = 35.31 \( \text{ft}^3/\text{s} \) (cubic feet per second)
  • ,
For our flow rate: \( 5.4 \text{ m}^3/\text{s} \)
Converting to liters per second: \( 5.4 \text{ m}^3/\text{s} \times 1000 = 5400 \text{ L/s} \)
Converting to cubic feet per second: \( 5.4 \text{ m}^3/\text{s} \times 35.31 = 190.67 \text{ ft}^3/\text{s} \)
These conversions help in situations where different units are required for analysis or presentation.

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Most popular questions from this chapter

A channel of symmetrical trapezoidal section, \(900 \mathrm{~mm}\) deep and with top and bottom widths \(1.8 \mathrm{~m}\) and \(600 \mathrm{~mm}\) respectively, carries water at a depth of \(600 \mathrm{~mm}\). If the channel slopes uniformly at 1 in 2600 and Chézy's coefficient is \(60 \mathrm{~m}^{1 / 2} \cdot \mathrm{s}^{-1}\), calculate the steady rate of flow in the channel.

Uniform flow occurs with a depth of \(900 \mathrm{~mm}\) in a rectangular prismatic channel \(2.5 \mathrm{~m}\) wide. If Manning's \(n=0.015\) and the bed slope is 1 in 1200 what is the minimum height of hump in the bed over which critical flow will be produced?

Ocean waves, with a period of \(8 \mathrm{~s}\) and amplitude \(0.6 \mathrm{~m}\) in deep water, approach the shore in the normal direction. A device \(80 \mathrm{~m}\) long for extracting power from the waves is installed parallel to the shore in water \(5 \mathrm{~m}\) deep. If there is negligible dissipation of energy before the waves reach the device and its efficiency is \(50 \%\), what power is produced? What is the amplitude of the waves immediately before this position? (Density of sea-water \(\left.=1025 \mathrm{~kg} \cdot \mathrm{m}^{-3} .\right)\)

A circular conduit is to satisfy the following conditions: capacity when flowing full, \(0.13 \mathrm{~m}^{3} \cdot \mathrm{s}^{-1}\); velocity when the depth is one quarter the diameter, not less than \(0.6 \mathrm{~m} \cdot \mathrm{s}^{-1}\). Assuming uniform flow, determine the diameter and the slope if Chézy's coefficient is \(58 \mathrm{~m}^{1 / 2} \cdot \mathrm{s}^{-1}\)

A venturi flume installed in a horizontal rectangular channel \(700 \mathrm{~mm}\) wide has a uniform throat width of \(280 \mathrm{~mm}\). When water flows through the channel at \(0.140 \mathrm{~m}^{3} \cdot \mathrm{s}^{-1}\), the depth at a section upstream of the flume is \(430 \mathrm{~mm}\). Neglecting friction, calculate the depth of flow at the throat, the depth at a section just downstream of the flume where the width is again \(700 \mathrm{~mm}\), and the force exerted on the stream in passing through the flume.

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