Application of Numerical Methods in Calculating the Depth of Submerged Ball in a RO Water System

Similar documents
Additional Information

Exam Question 9: Hydrostatics. March 6, Applied Mathematics: Lecture 8. Brendan Williamson. Introduction. Density, Weight and Volume

Fluid Mechanics - Hydrostatics. Sections 11 5 and 6

AP Lab 11.3 Archimedes Principle

Chapter 9 Fluids and Buoyant Force

Notes Chapter 3. Buoyancy

Ch. 4 Motion in One direction Ch 6. Pressure in Fluids and Atmospheric Pressure Ch. 7. Up-thrust in Fluids Ch. 8. Floatation and Relative Density

Fluids, Pressure and buoyancy

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Density, Pressure Learning Outcomes

PRESSURE AND BUOYANCY

Static Fluids. **All simulations and videos required for this package can be found on my website, here:

1. All fluids are: A. gases B. liquids C. gases or liquids D. non-metallic E. transparent ans: C

EXPERIMENT 8 BUOYANT FORCES

BUOYANCY, FLOATATION AND STABILITY

Density, Pressure Learning Outcomes

LECTURE 16: Buoyancy. Select LEARNING OBJECTIVES:

Lab 11 Density and Buoyancy

Nadia Naghi. Hung Do. Minh Lu. George Manoli PHYS Lab 12: Archimede s Principle. July 2, 2014

Section 3: Fluids. States of Matter Section 3. Preview Key Ideas Bellringer Pressure

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

Density and Specific Gravity

Physics 221, March 1. Key Concepts: Density and pressure Buoyancy Pumps and siphons Surface tension

mass of container full of air = g mass of container with extra air = g volume of air released = cm 3

Density and Buoyancy Notes

PHY131H1S - Class 23. Today: Fluids Pressure Pascal s Law Gauge Pressure Buoyancy, Archimedes Principle. A little pre-class reading quiz

10.4 Buoyancy is a force

L 13 Fluid Statics [2] More on fluids. How can a steel boat float. A ship can float in a cup of water! Today s weather

FLOATING AND SINKING

COURSE NUMBER: ME 321 Fluid Mechanics I Fluid statics. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET

HW #10 posted, due Thursday, Dec 2, 11:59 p.m. (last HW that contributes to the final grade)

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

Unit 1 Lesson 5 Fluids and Pressure. Copyright Houghton Mifflin Harcourt Publishing Company

Lecture 19 Fluids: density, pressure, Pascal s principle and Buoyancy.

Fluids always move from high pressure to low pressure. Air molecules pulled by gravity = atmospheric pressure

Float a Big Stick. To investigate how objects float by analyzing forces acting on a floating stick

LAB 7. ROTATION. 7.1 Problem. 7.2 Equipment. 7.3 Activities

FLUID STATICS II: BUOYANCY 1

To connect the words of Archimedes Principle to the actual behavior of submerged objects.

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

Chapter 15 Fluids. Copyright 2010 Pearson Education, Inc.

Quiz name: Chapter 13 Test Review - Fluids

Lecture 29 (Walker: ) Fluids II April 13, 2009

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Experiment P18: Buoyant Force (Force Sensor)

2015 EdExcel A Level Physics Topic 4. Density and upthrust

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Fluid Mechanics - Hydrostatics. AP Physics B

Chapter 15 Fluid. Density

Fluids. James H Dann, Ph.D. Say Thanks to the Authors Click (No sign in required)

EXPERIMENT (2) BUOYANCY & FLOTATION (METACENTRIC HEIGHT)

PHYS 101 Previous Exam Problems

Hydrostatics Physics Lab XI

Pressure is defined as force per unit area. Any fluid can exert a force

Page 1

Dec 6 3:08 PM. Density. Over the last two periods we discussed/observed the concept of density. What have we learned?

where ρ f is the density of the fluid, V is the submerged volume of the object, and g is the acceleration due to gravity.

Chapter 10 Fluids. Which has a greater density? Ch 10: Problem 5. Ch 10: Problem Phases of Matter Density and Specific Gravity

Motion, Forces, and Energy Revision (Chapters 3+4)

PHYS:1200 LECTURE 13 FLUIDS (2)

Lecture Outline Chapter 15. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Homework of chapter (3)

Fluid Statics. AP Physics 2

ARCHIMEDES PRINCIPLE AND THE COMPUTATION OF BUOYANT FORCES. Alexis Rodriguez-Carlson

LESSON 2: SUBMARINE BUOYANCY INVESTIGATION

FC-CIV HIDRCANA: Channel Hydraulics Flow Mechanics Review Fluid Statics

Density. Chapters 12-14: Phases of Matter. Example: Density. Conceptual Check. Springs 2/27/12. Mass Density vs. Weight Density

Name Class Date. (pp ) Write the letter of the correct answer in the space provided.

Buoyancy and Density. Buoyant Force and Fluid Pressure. Key Concept Buoyant force and density affect whether an object will float or sink in a fluid.

ConcepTest PowerPoints

Example A: A 400-N force is applied to a tabletop over a square area with side-length L = 20-cm.

1. The principle of fluid pressure that is used in hydraulic brakes or lifts is that:

Student Exploration: Archimedes Principle

More About Solids, Liquids and Gases ASSIGNMENT

17.2 and 17.3 Classifying Matter Liquids. Liquids

In the liquid phase, molecules can flow freely from position to position by sliding over one another. A liquid takes the shape of its container.

Density and Archimedes Principle 11-cor

Name. Student I.D.. Section:. Use g = 10 m/s 2

Vacuum P=0. h=76 cm A B C. Barometer

In the liquid phase, molecules can flow freely from position. another. A liquid takes the shape of its container. 19.

Concept of Fluid. Density. Pressure: Pressure in a Fluid. Pascal s principle. Buoyancy. Archimede s Principle. Forces on submerged surfaces

Chapter 9 Fluids CHAPTER CONTENTS

Slide 5 / What is the difference between the pressure on the bottom of a pool and the pressure on the water surface? A ρgh B ρg/h C ρ/gh D gh/ρ

Multiple Representations of Buoyancy. Meredith Weglarz, Jessica Oliveira, James Vesenka University of New England, Department of Chemistry and Physics

Properties of Fluids. How do ships float?

Chapter 14 Fluids Mass Density Pressure Pressure in a Static Fluid Pascal's Principle Archimedes' Principle

Review: Fluids. container into which it has been poured. changes gases are compressible. pressure changes

Lecture 20. Static fluids

Fluid Mechanics. Liquids and gases have the ability to flow They are called fluids There are a variety of LAWS that fluids obey

PHYSICS - CLUTCH CH 17: FLUID MECHANICS.

CHAPTER 9 Fluids. Units

North Carolina State University PY131 Lab Manual

Second Midterm Exam. Physics General Physics Lecture 20 - Fluids 11/9/2016. Fall 2016 Semester Prof. Matthew Jones

The density of a substance is the same for all samples of that substance.

Unit 7. Pressure in fluids

Irrigation &Hydraulics Department lb / ft to kg/lit.

Force Pressure = Area

Chapter 9 Solids and Fluids

Physics 1021 Experiment 4. Buoyancy

Chapter 9. Forces and Fluids

Transcription:

Research Article IJCRR Section: General Science Sci. Journal Impact Factor 4.016 ICV: 71.54 Application of Numerical Methods in Calculating the Depth of Submerged Ball in a RO Water System T. N. Kavitha 1, L. Shanmugasundaram 2 1 Assistant Professor of Mathematics, SCSVMV University, Kanchipuram, India; 2 Research schoiar, Department of Mathematics, SCSVMV University, Kanchipuram, India. ABSTRACT Objectives: In this work we use the bisection method through MATLAB for finding the depth of a submerged ball in a RO water tank. Material and Method: Using MATLAB, and by Bisection method, we find the depth of the submerged ball in a RO water system. Results: We know that Buoyancy (upthrust) is an upward force exerted by a fluid that opposes the weight of an immersed object. Archimedes principle indicates that the upward buoyant force that is exerted on a body immersed in a fluid, whether fully or partially submerged, is equal to the weight of the fluid that the body displaces and it acts in the upward direction at the centre of mass of the displaced fluid. Using this principle we have formed the polynomial equation, according to the radius of the ball submerged in water. We have solve this polynomial equation using MATLAB, and by Bisection method. This gives us the depth of the submerged ball in a RO water system. Conclusion: The polynomial equation in x we formed is a nonlinear equation. Solving it would give us the value of x, that is, the depth to which the floatball is submerged under water. Key Words: MATLAB, Buoyancy force, Archimedes Principle, Bisection method INTRODUCTION The main goals of this work is to introduce the concepts of numerical methods and introduce Matlab in an Engineering framework. By this we do not mean that every problem is a real life Engineering application, but more that the engineering way of thinking is emphasized throughout discussion. In a RO water tank we are opening the tank frequently to check the water level means, there is no use of the RO system, because the water get spoiled due to outside dust. So, we have to fix a water level checker. This should maintain the water level without opening the tank. So that we have use Plastic float ball and that automatically start and stop water flow. The float is adjustable to allow you to control the water height. In the Newest Reverse Osmosis System a Adjustable Mini Float Ball Valve can Shut off the water in the automatic Fill Feed Fish Tank Aquarium RO Water. We have to find the depth of the ball which is submerged in water. The permeate water then enters the storage tank. The tank level is controlled by a float switch, which turns the RO unit as well as the Spectra guard pump on and off. After the pressure tank, the water is re- pressurized by a pump and sent to the home usage. In this case we have to decide the water level height and fixing of lid in the tank, for that we should find depth of the ball using the bisection method. PRELIMINARIES Definition Buoyancy ( upthrust) is an upward force exerted by a fluid that opposes the weight of an immersed object. Corresponding Author: T. N. Kavitha, Assistant Professor of Mathematics, SCSVMV University, Kanchipuram, India. ISSN: 2231-2196 (Print) ISSN: 0975-5241 (Online) Received: 12.02.2017 Revised: 01.04.2017 Accepted: 20.04.2017 Int J Cur Res Rev Vol 9 Issue 10 May 2017 58

Definition The weight of the displaced fluid is directly proportional to the volume of the displaced fluid (if the surrounding fluid is of uniform density). The weight of the object in the fluid is reduced, because of the force acting on it, which is called upthrust. Archimedes principle Archimedes principle indicates that the upward buoyant force that is exerted on a body immersed in a fluid, whether fully or partially submerged, is equal to the weight of the fluid that the body displaces and it acts in the upward direction at the centre of mass of the displaced fluid. Archimedes principle is a law of physics fundamental to fluid mechanics. It was formulated by Archimedes of Syracuse. In a column of fluid, pressure increases with depth as a result of the weight of the overlying fluid. Thus the pressure at the bottom of a column of fluid is greater than at the top of the column. Similarly, the pressure at the bottom of an object submerged in a fluid is greater than at the top of the object. This pressure difference results in a net upwards force on the object. The magnitude of that force exerted is proportional to that pressure difference, and (as explained by Archimedes principle) is equivalent to the weight of the fluid that would otherwise occupy the volume of the object, i.e. the displaced fluid. In on Floating Bodies, Archimedes suggested that, Any object, wholly or partially immersed in a fluid, is buoyed up by a force equal to the weight of the fluid displaced by the object. For a fully submerged object, Archimedes principle can be reformulated as follows: Apparent immersed weight = weight of object weight of displaced fluid then inserted into the quotient of weights, which has been expanded by the mutual volume densityofobject densityoffluid = weight weightofdisplacedfluid yields the formula below. The density of the immersed object relative to the density of the fluid can easily be calculated without measuring any volumes: densityofobject densityoffluid = weight weight apparentimmensedweight Example: If you drop wood into water, buoyancy will keep it afloat. TO FIND THE DEPTH TO WHICH THE BALL WILL GET SUBMERGED WHEN FLOATING IN WATER In a RO water tank we are opening the tank frequently to check the water level means, there is no use of the RO system, because the water get spoiled due to outside dust. So, we have to fix a water level checker. This should maintain the water level without opening the tank. So that we have use Plastic float ball and that automatically start and stop water flow. The float is adjustable to allow you to control the water height. In the newest reverse osmosis system a adjustable mini float ball valve can shut off the water in the automatic fill feed fish tank aquarium RO water. We have to find the depth of the ball which is submerged in water. The permeate water then enters the storage tank. The tank level is controlled by a float switch, which turns the RO unit as well as the Spectra guard pump on and off. After the pressure tank, the water is re- pressurized by a pump and sent to the home usage. Suppose A ball has a gravity of 0.8 and has a radius of 6 cm is floating in water. We are trying to find the depth of the ball which the ball will get submerged when floating in water. According to Newton s third law of motion, every action has an equal and opposite reaction. In this case, the weight of the ball is balanced by the buoyancy force. Weight of ball = Buoyancy force (1) The weight of the ball is given by Weight of ball = (volume of ball) x(density of ball) x(acceleration due to gravity) 4 πr 3 3 = ( ρ )( g) b Where R = radius of ball(m), ρ = density of ball (kg/m 3 ), g = acceleration due to gravity(m/s 2 ). The buoyancy force is given by Buoyancy force = Weight of water displaced = (Volume of ball under water)(density of water)(acceleration due to gravity) π X 3 2 x R ρwg where x = depth to which ball is submerged, r w = density of water. (2) (3) 59 Int J Cur Res Rev Vol 9 Issue 10 May 2017

DERIVATION OF THE FORMULA FOR THE VOLUME OF A BALL SUBMERGED UNDER WATER. How do you find that the volume of the ball submerged under water as given by h 2 (3 r h) V π 3 = (4) where r = radius of the ball, h = height of the ball to which the ball is submerged. From calculus r V = Adx (5) r h where A is the cross-sectioned area at a distance x from the center of the sphere. The lower limit of integration is x= r- h as that is where the water line is Figure 2 - Deriving the equation for volume of ball under water and the upper limit is r as that is the bottom of the sphere. So, what is the A at any location x. From Figure 2, for a location x, OB = x, OA = r, Then AB = OA 2 - OB 2 = r 2 - x 2. (6) and AB is the radius of the area at x. So at location B is So A = π (AB) 2 = π(r 2 -x 2 ) (7) Where the specific gravity g b of the ball is given by g b = ρb ρ g b = 0.8cm = 0.008m w R = 6 cm = 0.06m Substituting in equation (4), we get 4(0.06) 3 (0.008) - 3 x 2 (0.06) + x 3 = 0 691 x 10-6 - 0.18 x 2 + x 3 = 0 This equation is a nonlinear equation. Solving it would give us the value of x, that is, the depth to which the floatball is submerged under water. The equation that gives the depth x to which the ball is submerged under water is given by SOLUTION USING BISECTION METHOD Use the bisection method of finding roots of equations to find the depth x to which the ball is submerged under water. Conduct three iterations to estimate the root of the above equation. Find the absolute relative approximate error at the end of each iteration, and the number of significant digits at least correct at the end of each iteration. From the physics of the problem, the ball would be submerged between x = 0 and x = 2R, where R = radius of the ball, that is 0 x 2R (9) 0 x 2(0.06) 0 x 0.12 Now substituting Equations (2) and (3) in Equation (1), Solution: Let us assume that the root of x 3 x 2 6 between [0,0.12] We find the solution using bisection method 0.18 + 691 10 = 0 lies Here we are going to use the MatLab for solving the same polynomial equation. In this procedure we have find the solution with a graph easily. Int J Cur Res Rev Vol 9 Issue 10 May 2017 60

CONCLUSION We find the depth of the submerged ball into the water using the buoyancy force and by the bisection method, Matlab is very helpful on finding the solution. The polynomial equation in x we formed is a nonlinear equation. Solving it would give us the value of x, that is, the depth to which the floatball is submerged under water. REFERENCES 1. Autar Kaw, Bisection method of solving a nonlinear equation, A text book, Bisection method of solving a nonlinear equation- 2007. 2. Web link: https://en.wikipedia.org/wiki/archimedes%27_principle 3. Ref: A dictionary of computing 2004 originally published by oxford University press 2004. Table 1: Below table contains ten iterations of the function. Figure 1: Depth to which the ball is submerged in water. Figure 2: Deriving the equation for volume of ball under water and the upper limit is r as that is the bottom of the sphere. So, what is the A at any location x. 61 Int J Cur Res Rev Vol 9 Issue 10 May 2017

Figure 3: Free Body Diagram showing the forces acting on the ball all immersed in water. Int J Cur Res Rev Vol 9 Issue 10 May 2017 62