Equilibrium of Strings

Slides:



Advertisements
Similar presentations
Forces in Beams and Cables
Advertisements

CIVL3310 STRUCTURAL ANALYSIS
Hanging Cables Consider a portion of cable At lowest point of cable, a horizontal force H acts to stop the cable moving to the right H W(x) At centre of.
Mechanics M2 Exam Questions. Click to go straight to a particular topic Moments Centre of Mass Collisions Work Energy Power Kinematics (Vectors) Work.
1 Chapter 7 Length of flange Introduction As the bending moment decreases towards the support, the flange plate may be varied and a smaller flange.
Teach A Level Maths Moment of a Force. Volume 4: Mechanics 1 Moment of a Force Volume 4: Mechanics 1 Moment of a Force.
CHAPTER 6 BENDING.
Forces in Beams and Cables
Copyright © 2011 Pearson Education South Asia Pte Ltd
BFC (Mechanics of Materials) Chapter 2: Shear Force and Bending Moment
Copyright © 2010 Pearson Education South Asia Pte Ltd
Engineering Mechanics: Statics
MECHANICS OF MATERIALS 7th Edition
Beams, Shear Force & Bending Moment Diagrams
7.4 Cables Flexible cables and chains are used to support and transmit loads from one member to another In suspension bridges and trolley wheels, they.
Rigid Bodies II: Equilibrium
Copyright © 2010 Pearson Education South Asia Pte Ltd
ENT 153 TUTORIAL 1.
Engineering Mechanics: Statics
EQUILIBRIUM OF PARTICLES
Slide #: 1 Chapter 4 Equilibrium of Rigid Bodies.
EQUILIBRIUM OF CONCURRENT COPLANAR FORCE SYSTEMS CONTENTS: 1] BASIC CONCEPTS: (a) Definition & Conditions for Equilibrium (b) Space Diagram & Free Body.
7.3 Relations between Distributed Load, Shear and Moment
VECTOR MECHANICS FOR ENGINEERS: STATICS Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University CHAPTER.
Chapter 3 Equilibrium of a Particle. 3.1 Condition for the Equilibrium of a Particle o "static equilibrium" is used to describe an object at rest. o To.
Bölüm 7 Çubuk ve Kablolarda Kuvvetler
1 INTRODUCTION The state of stress on any plane in a strained body is said to be ‘Compound Stress’, if, both Normal and Shear stresses are acting on.
1. The following diagram shows a system of forces acting on a particle in a plane. A third force is added so that the particle rests in equilibrium. Find.
CED, UET, Taxila 1 Arches Theory of Structure - I.
A push or pull on an object caused by its interaction with another object. Measured in NEWTONS (N)
1 George Washington Bridge 本章简要介绍索的特性和分析方法,主要包括索的特征、 索内力的变化、重力(竖向荷载作用下索的分析、广义索定 理以及确定索状拱的方法。与桁架相比,索只能承受轴向拉 力,内力单一,但必须形成一定的曲线才能承受不与索轴重 合的荷载,使其构成和分析独具特色。将索变形限定在较小.
The Mechanics of Forces
Forces in Beams and Cables
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS Objectives: a) Identify support reactions, and, b) Draw a free-body diagram.
PRESENTED BY Prof. Hanuamanth Raj Department of Mechanical Engineering, Sahaydri College of Engineering, Adyar Mangalore SHEAR FORCE AND BENDING MOMENT.
Mechanics of Solids (M2H321546)
X, Y axis (Horizontal & Vertical)
Structural Analysis 7th Edition in SI Units
Equilibrium of Rigid Bodies
Pure Bending.
Equilibrium of Rigid Bodies
Equilibrium of Coplanar- Concurrent force systems
Shear Force and Bending Moment Diagrams [SFD & BMD]
Dynamics of a Particle moving in a Straight Line
Student misconceptions
Arches Theory of Structure - I.
Moment of a force with respect to a point:
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Statically Determine of Beams and Frames
Chapter 7 FORCES IN BEAMS AND CABLES
Equilibrium of Rigid Bodies
Equilibrium of Rigid Bodies
Equilibrium Of a Rigid Body.
Moments.
Assignment 1 Determine magnitude and direction of resultant force of the following problems.
Equilibrium of Rigid Bodies
Applying Forces AP Physics 1.
Dr. L. BENEDICT MICHAEL RAJ HEAD & ASSOCIATE PROFESSOR
Engineering Mechanics: Statics
Applying Forces AP Physics C.
Chapter 5 Equilibrium of Forces. Chapter 5 Equilibrium of Forces.
Moments and Their Applications
Applications of Friction
Parallel Forces and Couples
Analysis of Perfect Frames (Analytical Method)
Analysis of Perfect Frames (Graphical Method)
Chapter 12 Support Reactions. Chapter 12 Support Reactions.
Analysis of Perfect Frames (Graphical Method)
Chapter 12 Support Reactions. Chapter 12 Support Reactions.
Composition and Resolution of Forces
Presentation transcript:

Equilibrium of Strings Chapter 15 Equilibrium of Strings

Learning Objectives Introduction Shape of a Loaded String Tension in a String Tension in a String Carrying Point Loads Tension in a String Carrying Uniformly Distributed Load Tension in a String when the Two Supports are at Different Levels Length of a String Length of a String when the Supports are at the Same Level Length of a String when the Supports are at Different Levels The Catenary

Shape of a Loaded String Introduction A string (or rope), in its theoretical sense, is absolutely flexible, light (i.e. its weight is neglected) and inextensible. It is capable of offering only tensile resistance. The slope of a loaded string depends upon its length and the loads supported by it. It will be interesting to know that if the loads carried by the string are changed (in magnitude or position) its shape will also change. Shape of a Loaded String Consider a string or cable suspended at two points A and B at the same level, and carrying a uniformly distributed load over its horizontal span as shown in Fig 15.1. Fig. 15.1.

Let w = Uniformly distributed load per unit length, l = Span of the cable, and yc = Central dip of the cable. Now consider any point (P) on the string. Let the coordinates of this point be x and y with respect to C, the lowest point of the string as origin. Now draw the tangent at P. Let q be the inclination of the tangent with the horizontal as shown in the figure. We know that the portion CP of the string is in equilibrium under the action of the following forces : Load (w.x) acting vertically downwards, Horizontal pull (H) acting horizontally at C, and Tension (T) acting at P along the tangent. Resolving the forces vertically and horizontally,

Tension in a String The determination of tension in the string or cable is one of the important criterion for its design. As a matter of fact, the tension in a string depends upon the magnitude and type of loading as well as levels of the two supports. Though there are many types of strings and loadings, yet the following are important from the subject point of view : String Carrying Point Loads String Carrying Uniformly Distributed Load String Supported at Different Levels

Tension in a String Carrying Point Loads Fig. 15.2 Consider a string or cable suspended at two points A and B at the same level and carrying point loads W1, W2 and W2 at C, D and E respectively. Let us assume the weight of the string to be negligible as compared to the point loads and the cable to take the shape as shown in Fig. 15.2. Let T1 = Tension in the string AC, T2 = Tension in the string CD, T3 = Tension in the string DE, and T4 = Tension in the string EB. Since all the points of the cable are in equilibrium, therefore vector diagram with the help of loads W1, W2, W3 as well as tensions T1, T2, T3 and T4 in the cable must close. Now draw the vector diagram for the given loads and tensions as shown in Fig. 15.2.(b) and as discussed below :

Select some suitable point p and draw a vertical line pq equal to the load W1 to some suitable scale, Similarly, draw qr, rs equal to loads W2 and W3 to the scale. Through p, draw a line parallel to AC and through q draw a line parallel to CD, meeting the first line at o. Join or and os. Now the vector diagram is given by the figure pqrsop. Through o, draw om perpendicular to the load line pqrs. The vertical reactions at A and B are given by pm and ms respectively to the scale. Now the tensions in the cable AC (T1), CD (T2), DE (T3) and EB (T4) are given by the lengths op, oq, or and os respectively to the scale. And the horizontal thrust is given by om to the scale. Example Three loads of 10 kN, 15 kN and 20 kN are suspended from a string AB as shown in Fig. 15.3. If the point D is at a depth of 3 m from the supports, find (i) vertical reactions at A and B ; (ii) horizontal thrusts at A and B ; (iii) sag of points C and E ; and (iv) tensions in all the segments of the string.

Tension in a String Carrying Uniformly Distributed Load Consider a string or cable suspended at two points A and B at the same level and carrying a uniformly distributed load over the horizontal span of the cable as shown in Fig. 15.5.

Example A suspension bridge of 40 m span with 1.5 m wide platform is subjected to an average load of 20 kN/m2. The bridge is supported by a pair of cables having a central dip of 5 m. Find the necessary cross sectional area of the cable, if the maximum permissible strees in the cable material is not to exceed 1050 N/mm2.

Tension in a String Supported at Different Levels Fig. 15.6. Tension in string ACB. Consider a string or cable ACB, supported at different levels at A and B, and carrying a uniformly distributed load as shown in Fig 15.6. Let C be the lowest point of the cable. Let w = Uniformly distributed load per unit length of the span, l = Span of the string, yc = Depth of the lowest point of the string C, from the lower support B, d = Difference between the levels of the two supports, l1 = Horizontal length between A and C, and l2 = Horizontal length between C and B.

Since the string is supporting vertical loads only, therefore the horizontal thrust at A, must be equal to the horizontal thrust at B. In order to locate position of the lowest point C, let us imagine the portion CB of the string to be extended to CB1, such that the new support B1 is at the same level as that of A. Similarly, imagnie the portion AC of the string to be cut short to A1C, such that the new support A1 is at the same level as that of B. From the geometry of the figure, we find that the string ACB1 has a span of 2l1 and a central dip of (yc + d) ; whereas A1CB has a span of 2l2 and a central dip of yc. Now in the string ACB1 the horizontal thrust

Length of a String It means the actual length of a string or cable required between two supports, when it is loaded when it is loaded with a uniformly distributed load and hangs in the form of a parabola. Here we shall discuss the following two cases : When the supports are at the same level When the supports are at different levels Length of a String when the Supports are at the Same Level Consider a string ACB supported at A and B at the same level, and carrying a uniformly distributed load as shown in Fig 15.9. Let C be the lowest point of the cable.

Example A steel wire, of uniform section, is hung in the form of a parabola. Find the maximum horizontal span, if the central dip is 1/12th of the span and the strees in steel wire is not to exceed 120 N/mm2. Take mass density of the steel as 7800 kg/m3.