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Beam:
Beam is a structural member subjected
to lateral loads, that is, forces or moments
having their vectors perpendicular to the axis
of the bar.
Types of Beams:
Beams are usually classified by the manner in which they are supported
๏ฑSimply supported beam
๏ฑCantilever beam
๏ฑOver hanged beam
๏ฑContinuous beam
๏ฑPropped cantilever beam
๏ฑFixed beam
Simply supported beam
A beam with a pin support at one end and a roller support at the other is called a
simply supported beam or a simple beam.
Cantilever beam
A beam which is fixed at one end and free at the other, is called a cantilever
beam.
Over hanged beam
This beam is simply supported at points A
and B but it also projects beyond the
support at B.
Statically Indeterminate Beams
Continuous beam Propped cantilever beam
Fixed beam
Support Reactions:
๏ฑThe essential feature of a pin support is that
it prevents translation at the end of a beam
but does not prevent rotation. Thus, end A of
the beam of Fig cannot move horizontally or
vertically but the axis of the beam can rotate
in the plane of the figure.
๏ฑA pin support is capable of developing a force
reaction with both horizontal and vertical
components (HA and RA), but it cannot
develop a moment reaction.
Simply supported beam
Support Reactions:
๏ฑAt end B of the beam the roller support
prevents translation in the vertical direction
but not in the horizontal direction; hence this
support can resist a vertical force (RB) but not
a horizontal force. Of course, the axis of the
beam is free to rotate at B just as it is at A.
Simply supported beam
Support Reactions at pin end and roller end:
Simply supported beam
Support Reactions:
Cantilever beam
๏ฑAt the fixed support (or clamped support) the
beam can neither translate nor rotate,
whereas at the free end it may do both.
Consequently, both force and moment
reactions may exist at the fixed support.
Support Reactions at fixed end:
Cantilever beam
Types of loads:
๏ฑ When a load is applied over a very small area it may be idealized as a concentrated load, which is a single
force.
๏ฑ When a load is spread along the axis of a beam, it is represented as a distributed load.
๏ฑ A uniformly distributed load, or uniform load, has constant intensity q per unit distance.
๏ฑ A varying load has an intensity that changes with distance along the axis; for instance, the linearly
varying load has an intensity that varies linearly from q1 to q2.
๏ฑ Another kind of load is a couple
Calculation of Support Reactions:
Q1. Calculate the support reactions for the beam as shown in the figure
Calculation of Support Reactions:
Free body diagram of the
beam
Calculation of Support Reactions:
Free body diagram of the beam
๐œฎ๐‘ญ ๐’™ = ๐ŸŽ
โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ
๐œฎ๐‘ญ ๐’š = ๐ŸŽ
๐‘ ๐‘จ + ๐‘น ๐‘ฉ โˆ’ ๐Ÿ‘ โ‹… ๐Ÿ“ โˆ’ ๐Ÿ• = ๐ŸŽ
๐‘ ๐‘จ + ๐‘น ๐‘ฉ =10.5
๐›ด๐‘€๐ด = 0
-3.5 *(0.8)- 7 * (1.2+.8) +RB *3=0
๏ƒž RB=( 3.5 *0.8 + 7 *2)/3
๏ƒž RB = 5.6 kN
โ†’ (1)
โ†’ (2)
Substitute (2) in (1)
RA = 10.5- RB
RA = 10.5- 5.6 = 4.9 kN.
Q3. Calculate the support reactions for the beam as shown in the figure
Free body diagram of the beam
๐œฎ๐‘ญ ๐’™ = ๐ŸŽ
โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ
๐œฎ๐‘ญ ๐’š = ๐ŸŽ
๐‘ ๐‘จ + ๐‘น ๐‘ฉ โˆ’ ๐Ÿ” โˆ’ ๐Ÿ โˆ— ๐Ÿ. ๐Ÿ“ = ๐ŸŽ
๐‘ ๐‘จ + ๐‘น ๐‘ฉ = ๐Ÿ—
๐›ด๐‘€๐ด = 0
-6 *(1)- 2 *1.5 * (2.5+.75) + RB *4=0
๏ƒž RB=( 6+ 2*1.5 * 3.25)/4
๏ƒž RB = 3.94 kN
โ†’ (1)
โ†’ (2)
Substitute (2) in (1)
RA = 9- RB
RA = 9- 3.94= 5.06 kN.
Q4. Calculate the support reactions for the beam as shown in the figure
Free body diagram of the beam
๐œฎ๐‘ญ ๐’™ = ๐ŸŽ
โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ
๐œฎ๐‘ญ ๐’š = ๐ŸŽ
๐‘ ๐‘จ โˆ’ ๐Ÿ’ โˆ’ ๐Ÿ. ๐Ÿ“ โˆ— ๐Ÿ = ๐ŸŽ
๐‘ ๐‘จ = ๐Ÿ• ๐ค๐
๐›ด๐‘€ ๐น๐ธ = 0
- ๐‘€๐ด โˆ’ 4*(1)- 1.5 *2 * (2 +1 ) =0
๏ƒž ๐‘€๐ด =- ( 4+ 1.5 *2 * 3)
๏ƒž ๐‘€๐ด = - 13 kN-m
๏ฑ Finding the reactions is usually the first step in the analysis of a beam.
๏ฑ Once the reactions are known, the shear forces and bending moments can be found. If a beam is
supported in a statically determinate manner, all reactions can be found from free-body diagrams and
equations of equilibrium.
๏ฑ Internal stress resultants: Shear forces and bending moments are the resultants of stresses distributed
over the cross section. Therefore, these quantities are known collectively as stress resultants. The stress
resultants in statically determinate beams can be calculated from equations of equilibrium.
๏ฑ When designing a beam, we usually need to know how the shear forces and bending moments vary
throughout the length of the beam. Of special importance are the maximum and minimum values of
these quantities. Information of this kind is usually provided by graphs in which the shear force and
bending moment are plotted as ordinates and the distance x along the axis of the beam is plotted as
the abscissa. Such graphs are called shear-force and bending-moment diagrams.
Q5. Calculate the support reactions for the beam as shown in the figure

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Beams Introduction

  • 1.
  • 2. Beam: Beam is a structural member subjected to lateral loads, that is, forces or moments having their vectors perpendicular to the axis of the bar.
  • 3. Types of Beams: Beams are usually classified by the manner in which they are supported ๏ฑSimply supported beam ๏ฑCantilever beam ๏ฑOver hanged beam ๏ฑContinuous beam ๏ฑPropped cantilever beam ๏ฑFixed beam
  • 4. Simply supported beam A beam with a pin support at one end and a roller support at the other is called a simply supported beam or a simple beam.
  • 5. Cantilever beam A beam which is fixed at one end and free at the other, is called a cantilever beam.
  • 6. Over hanged beam This beam is simply supported at points A and B but it also projects beyond the support at B.
  • 7. Statically Indeterminate Beams Continuous beam Propped cantilever beam Fixed beam
  • 8. Support Reactions: ๏ฑThe essential feature of a pin support is that it prevents translation at the end of a beam but does not prevent rotation. Thus, end A of the beam of Fig cannot move horizontally or vertically but the axis of the beam can rotate in the plane of the figure. ๏ฑA pin support is capable of developing a force reaction with both horizontal and vertical components (HA and RA), but it cannot develop a moment reaction. Simply supported beam
  • 9. Support Reactions: ๏ฑAt end B of the beam the roller support prevents translation in the vertical direction but not in the horizontal direction; hence this support can resist a vertical force (RB) but not a horizontal force. Of course, the axis of the beam is free to rotate at B just as it is at A. Simply supported beam
  • 10. Support Reactions at pin end and roller end: Simply supported beam
  • 11. Support Reactions: Cantilever beam ๏ฑAt the fixed support (or clamped support) the beam can neither translate nor rotate, whereas at the free end it may do both. Consequently, both force and moment reactions may exist at the fixed support.
  • 12. Support Reactions at fixed end: Cantilever beam
  • 13. Types of loads: ๏ฑ When a load is applied over a very small area it may be idealized as a concentrated load, which is a single force. ๏ฑ When a load is spread along the axis of a beam, it is represented as a distributed load. ๏ฑ A uniformly distributed load, or uniform load, has constant intensity q per unit distance. ๏ฑ A varying load has an intensity that changes with distance along the axis; for instance, the linearly varying load has an intensity that varies linearly from q1 to q2. ๏ฑ Another kind of load is a couple
  • 14. Calculation of Support Reactions: Q1. Calculate the support reactions for the beam as shown in the figure
  • 15. Calculation of Support Reactions: Free body diagram of the beam
  • 16. Calculation of Support Reactions: Free body diagram of the beam ๐œฎ๐‘ญ ๐’™ = ๐ŸŽ โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ ๐œฎ๐‘ญ ๐’š = ๐ŸŽ ๐‘ ๐‘จ + ๐‘น ๐‘ฉ โˆ’ ๐Ÿ‘ โ‹… ๐Ÿ“ โˆ’ ๐Ÿ• = ๐ŸŽ ๐‘ ๐‘จ + ๐‘น ๐‘ฉ =10.5 ๐›ด๐‘€๐ด = 0 -3.5 *(0.8)- 7 * (1.2+.8) +RB *3=0 ๏ƒž RB=( 3.5 *0.8 + 7 *2)/3 ๏ƒž RB = 5.6 kN โ†’ (1) โ†’ (2) Substitute (2) in (1) RA = 10.5- RB RA = 10.5- 5.6 = 4.9 kN.
  • 17. Q3. Calculate the support reactions for the beam as shown in the figure
  • 18. Free body diagram of the beam ๐œฎ๐‘ญ ๐’™ = ๐ŸŽ โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ ๐œฎ๐‘ญ ๐’š = ๐ŸŽ ๐‘ ๐‘จ + ๐‘น ๐‘ฉ โˆ’ ๐Ÿ” โˆ’ ๐Ÿ โˆ— ๐Ÿ. ๐Ÿ“ = ๐ŸŽ ๐‘ ๐‘จ + ๐‘น ๐‘ฉ = ๐Ÿ— ๐›ด๐‘€๐ด = 0 -6 *(1)- 2 *1.5 * (2.5+.75) + RB *4=0 ๏ƒž RB=( 6+ 2*1.5 * 3.25)/4 ๏ƒž RB = 3.94 kN โ†’ (1) โ†’ (2) Substitute (2) in (1) RA = 9- RB RA = 9- 3.94= 5.06 kN.
  • 19. Q4. Calculate the support reactions for the beam as shown in the figure
  • 20. Free body diagram of the beam ๐œฎ๐‘ญ ๐’™ = ๐ŸŽ โ‡’ ๐‘ฏ ๐‘จ= ๐ŸŽ ๐œฎ๐‘ญ ๐’š = ๐ŸŽ ๐‘ ๐‘จ โˆ’ ๐Ÿ’ โˆ’ ๐Ÿ. ๐Ÿ“ โˆ— ๐Ÿ = ๐ŸŽ ๐‘ ๐‘จ = ๐Ÿ• ๐ค๐ ๐›ด๐‘€ ๐น๐ธ = 0 - ๐‘€๐ด โˆ’ 4*(1)- 1.5 *2 * (2 +1 ) =0 ๏ƒž ๐‘€๐ด =- ( 4+ 1.5 *2 * 3) ๏ƒž ๐‘€๐ด = - 13 kN-m
  • 21. ๏ฑ Finding the reactions is usually the first step in the analysis of a beam. ๏ฑ Once the reactions are known, the shear forces and bending moments can be found. If a beam is supported in a statically determinate manner, all reactions can be found from free-body diagrams and equations of equilibrium. ๏ฑ Internal stress resultants: Shear forces and bending moments are the resultants of stresses distributed over the cross section. Therefore, these quantities are known collectively as stress resultants. The stress resultants in statically determinate beams can be calculated from equations of equilibrium. ๏ฑ When designing a beam, we usually need to know how the shear forces and bending moments vary throughout the length of the beam. Of special importance are the maximum and minimum values of these quantities. Information of this kind is usually provided by graphs in which the shear force and bending moment are plotted as ordinates and the distance x along the axis of the beam is plotted as the abscissa. Such graphs are called shear-force and bending-moment diagrams.
  • 22. Q5. Calculate the support reactions for the beam as shown in the figure

Editor's Notes

  1. the reactions at the supports of the beam can be determined by the methods of statics. So it is statically determinate
  2. the reactions at the supports of the beam can be determined by the methods of statics. So it is statically determinate
  3. the reactions at the supports of the beam can be determined by the methods of statics. So it is statically determinate
  4. The reactions at the supports of the beams involve more than three unknowns and cannot be determined by the methods of statics alone. The properties of the beams with regard to their resistance to deformations must be taken into consideration. Such beams are said to be statically indeterminate