deflection of beam.doc

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Deflection of Beams INTRODUCTION Under the action of external loads, the beam is subjected to stresses and deformation at various points along the length. The deformation is caused due to bending moment and shear force. Since the deformation caused due to shear force in shallow beams is very small, it is generally neglected. Elastic Line: It is a line which represents the deformed shape of the beam. Hence, it is the line along which the longitudinal axis of the beam bends. Deflection: Vertical displacement measured from original neutral surface to the neutral surface of the deformed beam. Slope: Angle made by the tangent to the elastic curve with respect to horizontal

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Page 1: deflection of beam.doc

Deflection of Beams

INTRODUCTIONUnder the action of external loads, the beam is subjected to stresses and deformation at various points along the length. The deformation is caused due to bending moment and shear force. Since the deformation caused due to shear force in shallow beams is very small, it is generally neglected.

Elastic Line: It is a line which represents the deformed shape of the beam. Hence, it is the line along which the longitudinal axis of the beam bends.

Deflection: Vertical displacement measured from original neutral surface to the neutral surface of the deformed beam.

Slope: Angle made by the tangent to the elastic curve with respect to horizontal

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A designer has to decide the dimensions of beam not only based on strength requirement but also based on considering deflection. In mechanical components excessive deflection causes mis-alignment and non performance of machine. In building it give rise to psychological unrest and sometimes cracks in roofing materials. Deflection calculations are required to impose consistency conditions in the analysis of indeterminate structures

Strength: It is a measure of the resistance offered by the beam to load

Stiffness: It is a measure at the resistance offered by the beam to deformation. Usually span / deflection is used to denote the stiffness. Greater the stiffness, smaller the deflection. The term (EI) called “flexural rigidity” and is used to denote the stiffness.

Thus Moment of inertia in Case – II is 144 times higher than Case – I and hence more stiffer.

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Flexural Rigidity

The product of Young's modulus and moment of inertia (EI) is used to denote the flexural rigidity.

Differential Equation for Deflection Curve

Differential Equation for Deflection Curve

Let AB be the part of the beam which is bent into an arc of the circle. Let (x,y) be co-ordinates of A and (x + dx, y + dy) be the co-ordinates of B. Let the length of arc AB = ds. Let the tangents at A and B make angles q and ( q + d q ) with respect to x-axis.

We have

Differentiating both sides with respect of x;

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Since dy/dx is small, its square is still small, neglecting (dy/dx)2 ; we have

This is also known as Euler - Bernoulli's equation.

NOTE:

While deriving Y-axis is taken upwards Curvature is concave towards the positive y axis.

This occurs for sagging BM, which is positive.

Sign Convention

Bending moment Sagging + vc

If Y is +ve - Deflection is upwards  Y is –ve - Deflection is downwards If is +ve – Slope is Anticlockwise   is - ve – Slope is clockwise

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Methods of Calculating Deflection and Slope

Double Integration method Macaulay's method

Strain energy method

Moment area method

Conjugate Beam method

Each method has certain advantages and disadvantages.

Relationship between Loading,S.F,BM,Slope,and Deflection

Macaulay's Method

Rules

1. Take the origin on the extreme left. 2. Take a section in the last segment of the beam and calculate BM by considering left portion. 3. Integrate (x-a) using the formula

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4. If the expression (x-a)n becomes negative on substituting the value of x, neglect the terms containing the factor (x-a)n 5. If the beam carries UDL and if the section doesn't cuts the UDL, extend the UDL upto the section and impose a UDL in the opposite direction to counteract it. 6. If a couple is acting, the BM equation is modified as; M = R A x + M (x-a)0.

7. The constant C1 and C2 all determined using boundary conditions. a) S.S. Beam – Deflection is zero at supportsb) Cantilever – Deflection and slope are zero at support.

Standard Cases

Find deflection at C and slope at A

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Standard Cases (Contd.)

Boundary Condition

(i) at x = 0, y = 0 from eq. (2)   C2 = 0       (ii) at x = l, y = 0 from eq. (2)

Substitute C1 and C2 in (1) and (2)

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2. Determine deflection at centre and slope at end

Boundary Conditions

(i) at x = 0, y = 0 from (2) C2 = 0

(ii) at x = 0, y = 0 from (2)

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3. Determine deflection and slope at A

Boundary Condition

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4. Determine deflection and slope at A

Answer (Anticlockwise)

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Numerical Examples

1. A Simply Supported Beam of span 8m carries two concentrated load of 30kN each at 3m from each end. Find the maximum deflection and deflection under the load and maximum slope

Boundary Conditions

  (i) at x = 0; y = 0 From eq.(2) 0 = C2

  (ii) at x = 8; y = 0 ,

Again from eq. (2)

  C1 = -225

Substitute in (1) and (2)

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since beam is symmetrical, maximum deflection occurs at center

2. A Simply Supported Beam has a span of 6m and it carries two concentrated loads of 40kN and 10kN at a distance of 2m and 4m from left support. Find the deflection under 40 kN load. Also find the maximum deflection and slope. AssumeE = 200 GPa, I = 4 × 107 mm4

Boundary Conditions

Page 13: deflection of beam.doc

  (i) at x = 0; y = 0 Fromeq. (2) C2 = 0   (ii) at x = 6 ; y = 0

Substitute C1 and C2 in slope and deflection equation

Deflection under load

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Maximum deflection

NOTE:Since the Beam is not symmetrical, maximum deflection do not occur at centre, but it is generally occurs in the central region.

To determine the position, equate the slope equation in central region to zero.For central region, maximum value of x = 4

 

3. A Cantilever beam of 100 mm wick and 200 mm deep of span 2m is loaded with a UDL 5kN/m from the free end upto 1m. Find slope and deflection at free end E = 210 GPa

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Add and Remove UDL upto the section

Boundary Condition

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Solving the above two equations

C1 = – 5.82, C2 = – 8.52

Substituting C1 and C2 in eq. (1) and (2).

Note :

No need to extend the UDL.

4. A Simply Supported Beam of span 5m and EI = 40,000 kN-m2 is subjected to clockwise couple of 250 kN-m at a distance of 3m from left. Find the deflection at the point of application of couple. Find also the maximum deflection.

 

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Reactions RB = + 50 kN RA= – 50 kN

  

Boundary conditions

  i) at x = 0 ; y = 0 Form eq. 2 C2 = 0   ii) at x = 5; y = 0 Form eq. 2

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Maximum deflection

Maximum deflection is likely to occur in region AC.

Equating the slope equation to zero in region AC

  -25x2 + 108.3 = 0   x = 2.08m

 

NOTE: If slope expression in region BC is equate to 0.

  -25x2 + 250x – 750 + 108.3 = 0 Solving x 1 = 1.5 and x 2 = 8.4 (Invalid)

5. Determine the deflection at B slope at D, I = 1.6 × 107 mm4 E = 210 GPa.