Study on Wave calculation of an air cushion surge chamber

Slides:



Advertisements
Similar presentations
Lecture 9 - Flexure June 20, 2003 CVEN 444.
Advertisements

Lecture# 9 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES
Energy of the Simple Harmonic Oscillator
Information processing for model building of an electric power system, based on experimental data Kozmin Stanislav. State National Research Polytechnic.
Booster System Basics: Constant Speed Systems
Chapter 3.2: Heat Exchanger Analysis Using -NTU method
Istituto “Enrico Fermi” Mantova School Year Physics course The physics of sound.
Skyler Goldman, Meteorology, DMES RELATIONSHIP BETWEEN ROUGHNESS LENGTH, STATIC STABILITY, AND DRAG COEFFICIENT IN A DUNE ENVIRONMENT.
Numerical Hydraulics W. Kinzelbach with Marc Wolf and Cornel Beffa Lecture 3: Computation of pressure surges.
HYDRAULIC 1 CVE 303.
Chapter 16 Wave Motion.
Fluid Dynamics.
Elementary Fluid Dynamics: The Bernoulli Equation
CHE/ME 109 Heat Transfer in Electronics
Announcements Read Chapter 7 Quiz on HW 3 Today
Fluid Mechanics 06. Energy, Work and Power Work:- Work is force acting through a distance when the force is parallel to the direction of motion. Energy:-
EE535: Renewable Energy: Systems, Technology & Economics
Abstract An upgrade to the ATLAS silicon tracker cooling control system may require a change from C 3 F 8 (octafluoro-propane) to a blend containing 10-30%
Hydrodynamics.
1 CTC 450 Pumps Pumps
Airball Demo Modeling —— Dimensional Analysis Method Based on Genetic Algorithm for Key Parameters Identification Name : Zhisheng Team Advisor : Zhang.
Chapter 15B - Fluids in Motion
Basic Electrical Theory: Understanding Ohm’s Law Copyright © Texas Education Agency, All rights reserved.
1 Gases Chapter Properties of Gases Expand to completely fill their container Take the Shape of their container Low Density –much less than solid.
Pipe Networks Dr. Kristoph-Dietrich Kinzli Fall 2011 CWR 4540 C
Oscillations & Waves IB Physics. Simple Harmonic Motion Oscillation 4. Physics. a. an effect expressible as a quantity that repeatedly and regularly.
1 Chapter 6: The States of Matter. 2 PHYSICAL PROPERTIES OF MATTER All three states of matter have certain properties that help distinguish between the.
Power Plant Construction and QA/QC Section 7.2 – Dams, Spillways, Water Conductors and Power Houses Engineering Technology Division.
SIMULATION OF GAS PIPELINES LEAKAGE USING CHARACTERISTICS METHOD Author: Ehsan Nourollahi Organization: NIGC (National Iranian Gas Company) Department.
Wave – any disturbance that transmits energy through matter or space Medium – a substance through which a wave can travel. Can be a solid, liquid, or.
Double Pipe HEAT EXCHANGERS with Finned Inner Tube P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Ideas for Creation of Compact.
Computational fluid dynamics Authors: A. Ghavrish, Ass. Prof. of NMU, M. Packer, President of LDI inc.
Wednesday, Nov. 19, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #21 Wednesday, Nov. 19, 2003 Dr. Mystery Lecturer 1.Fluid.
Lesson Measuring and Calculating Electricity. Interest Approach § Have you or your parents ever been using several appliances in the kitchen and had a.
Reaction Rates Chapter 17 Honors Chemistry Red  Blue Reaction Rates.
Gas Laws A. The ____ _____ are simple mathematical relationships between the _______, _______, ___________, and __________ of a gas. gas laws pressure.
Hydraulics is defined as the study of fluid behavior, at rest and in motion Properly designed piping with sound hydraulics can: - Greatly reduce maintenance.
Air Resistance If you drop a feather and a cannonball at the same time, from the same height, which will hit the ground first? The cannonball of course.

MECH 322 Instrumentation Lab 6 Fluid Speed and Volume Flow Rate Performed: February 27, 2007 Group 0 Miles Greiner Lab Instructors: Mithun Gudipati, Venkata.
Chapter 12 Preview Objectives The Production of Sound Waves
ME 391 Instrumentation LAB #6 Volume Flow Rate and Centerline Speed in a Tube Wind Tunnel Performed: 03/05/2004 Soma: I believe I performed 50% of this.
Chapter Twenty-Three: Waves  23.1 Harmonic Motion  23.2 Properties of Waves  23.3 Wave Motion.
GOVERNMENT ENGINEERING COLLEGE, BHARUCH (014) Chemical Engineering department SEM-iii Sub: fluid flow operation topic: orifice meter & rotAmeter Guid by:
Chapter 12 Compressible Flow
Physics Mrs. Dimler SOUND.  Every sound wave begins with a vibrating object, such as the vibrating prong of a tuning fork. Tuning fork and air molecules.
CHARACTERISTICS OF WAVES Properties of Waves. WHAT ARE THE AMPLITUDE, WAVELENGTH, FREQUENCY, AND SPEED OF A WAVE?  Waves vary greatly.  Waves can be.
Introduction Results & Discussion At present, disinfection of wells and drinking water pipelines is carried out by treating with chlorine- containing reagents.
Sanitary Engineering Lecture 10 Revision
Enrollment No.Name Ketan Laiya Vipul Vasava Prepared by: Guided by Prof. M.J.Zinzuvadia.
Sanitary Engineering Lecture 7
Chapter 15B - Fluids in Motion
First Law of Thermodynamics applied to Flow processes
Waldemar Janicki, Adam Adamkowski
Chapter 1.
PHYS 1443 – Section 003 Lecture #21
Fluid Flow.
HYDRO ELECTRIC POWER PLANTS BY Prabhakaran.T AP/MECH
Find : Velocity V and discharge Q Problem 2
LAB #6 Volume Flow Rate and Centerline Speed in a Tube Wind Tunnel
Air Volume Flow Rate and Centerline Velocity in a Tube Wind Tunnel
TEM – Lecture 2 Basic concepts of heat transfer:
How does a gas differ from a solid and a liquid?
Fundamentals of Convection
Basic Electrical Theory: Understanding Ohm’s Law
For this type of flow, the stagnation temperature is constant, then
Conservation of Energy/Bernoulli’s Equation
Basic Chemistry Chapter 11 Gases Chapter 11 Lecture
Pumps and pumping station
Chapter Twenty-Three: Waves
Presentation transcript:

Study on Wave calculation of an air cushion surge chamber Xiaohong Zhang Xi’an University of Technology, Institute of Water Resources and Hydro-Electric Engineering, Xi’an,Shaanxi

Abstract. To constant flow, the varying rule between gaseous volume and pressure meets Boyle Gas Law. But, in transient process of water diversion system, kinetic characteristic of the gas in air cushion surge chamber has certain complexity when there is great fluctuation in surge chamber.

Therefore, when computing surge of air cushion surge chamber, firstly, it is necessary that gaseous volume and pressure meet actual rule and important to establish correct mathematic model. Secondly, initial height and pressure of the chamber should be confirmed correctly.

Then the computing method of water level surge of air cushion surge chamber is acquired. The basic equations and boundary conditions of the surge chamber were established in this article. Parameters selection, structure design and surge calculation of the air cushion surge chamber were conducted.

The effect of the initial air height and Polytrophic Exponent n in the chamber on the fluctuations of pressure and changes of water level is discussed. The results are quite important to fluid transient study of the air cushion surge chamber and may promote its use in water power plant.

1.Basic equations of the transient flow in Pressure pipelines 1.1 motion equation and continuity equation

1.2 Characteristic equation and its differential form

Differential form of Characteristic equations:

2.Surge chamber boundary conditions Boundary conditions of air cushion surge chamber are showed in Figure 1. Fig. 1..Boundary conditions of Air Cushion Surge Chamber

equation:

HP1,NS,、QP1,NS, QP2,1,、Z,、QC,、P, and L are seven unknown parameters in t moment when calculating water hammer pressure and surge chamber fluctuations jointly. The air pressure change, water level fluctuation and other physical parameters can be determined by solving the boundary equations of the chamber jointly.

3 Examples and results analysis A hydropower station has 100 meters high roller compacted concrete arch dam. The total installed capacity is 3×2.4 million watt. The entire power generation system consists of water intake tower, diversion tunnel, surge chamber, pressure pipeline fork tubes and branch pipe. The hydropower station design discharge is 93m3/s, design head is 90m, maximum flood level is 512.5m, dead water level is 485m,

pressure diversion tunnel is 2715 pressure diversion tunnel is 2715.213m long (to centerline of surge chamber), tunnel centerline elevation near surge chamber is 463.524 meters, and tunnel diameter after lined is 6.0m. Considering the terrain and environmental protection requirements, air-cushion type surge chamber is designed. After the chamber is buried pressure pipe with 5.5 meters inner diameter and 134.281 meters long main pipeline. The main pipe divided into three 3.0m inner diameter branches before enter the main power house and the distance between them is about 102 meters.

3.1 Results analysis of air-cushion surge chamber calculation 3.2.1 Influence of initial heights to the pressure and surge of air cushion surge chamber In order to compare and show the relationship between initial height and surge of air chamber , L0 is chose as 10 m (L0/24=0.42), 12m (L0/24=0.50) and 16 meters(L0/24=0.67) respectively, and partial results are showed in Table 1, Figure 2, and Figure 3.

Fig. 2. Fluctuation Course of Surge in air cushion Surge Chamber (Lo=10m, n=1.4)

Fig. 3. Fluctuation Course of Pressure in air cushion Surge Chamber (Lo=10m, n=1.4)

Table 1. Surge Water Level When Three Sets Discard all Loads at the same time in Air Cushion Surge Chamber

Based on calculation, It was found that under the same calculation conditions, same surface area of surge chamber, and same polytrophic exponent, with different initial height or a different initial pressure of air chamber (volume), the highest surge (maximum pressure chamber) comes in quite close time with different value, and has some rules.

It shows that the lower the initial air chamber height Lo the higher the maximum and minimum swell height of air chamber, and vice versa. Therefore increasing the initial pressure can reduce the height of the air chamber and the total amount of excavation. However, increase of the initial pressure is restricted by the minimum water level of air chamber. Air is not allowed to enter the diversion tunnel.

In air cushion surge chamber the existence of "air cushion" buffer the effects of water level fluctuations. Its water level fluctuation differs to the conventional normal open chamber. When the hydropower station load change, water level fluctuations of the conventional open surge chamber likes sine wave attenuation curve, but the water level fluctuations of air cushion surge chamber have the following characteristics: water level fluctuation waveform has steep wave crest and mild trough. It can be clearly seen from fig.3

that the amplitude of water level fluctuation of air cushion surge chamber is smaller than that of the conventional open surge chamber. While along with continuing fluctuation time, the attenuation speed is slower than that of conventional open surge chamber.

3.2.2 The impact of polytrophic exponent n on the pressure and surge of air cushion surge chamber The indoor air cushion surge chamber characteristics ranges from constant temperature and adiabatic process in the transition process. In order to illustrate the impact of different states of the transition process, a different combination of n value is calculated.

Fig. 4.Fluctuation Course of the maximum pressure of air cushion surge chamber with index n

5 Conclusion Through a real example this article is about more in-depth study on air cushion surge chamber fluctuations in the course of several main parameters and the relationship between them, shows the range of initial height L0 of air cushion surge chamber (initial air surge chamber pressure P0), and polytrophic exponent n. That has great important influence to the application of air cushion surge chamber in China.

Thank you