π₯SSC JE Very IMP One liners:
π΄1st derivative of deflection(β)gives slope(ΞΈ)
π΄2nd derivative of deflection(β) gives moment(M)
π΄ 3rd derivative of deflection(β) gives shear force(S)
π΄ 4th derivative of deflection(β) gives intensity of loading(W)
π΄Slope of bending moment diag. gives shear force
π΄Negative slope of shear force diag. gives loading intensity
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π΄1st derivative of deflection(β)gives slope(ΞΈ)
π΄2nd derivative of deflection(β) gives moment(M)
π΄ 3rd derivative of deflection(β) gives shear force(S)
π΄ 4th derivative of deflection(β) gives intensity of loading(W)
π΄Slope of bending moment diag. gives shear force
π΄Negative slope of shear force diag. gives loading intensity
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π₯9π4
The kern of a section is the region in which a compressive point load may be applied without producing any tensile stress on the cross section.
β Shape of KERN in eccentric loading -
Column section Kern shape
Rectangular Rhombus
Square Square
Circular Circle
I section Rhombus
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π5β€3π1π±1π€©1
SHEAR CENTRE-
β Shear centre - a point from which a concentrated load passes but there will be only bending and no twisting.
β It is also called as centre of of flexure.
β Resultant of shear passes through shear centre.
β Shear centre always lies on axis of symmetry if exists.
β Shear centre (e) for various sections
Channel => e = bΒ²hΒ²t / 4I
Semicircular => e = 4R / 3.14
Open circular slit => e = 2R
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π8β‘3π―3π₯2π±2
( Theory of simple bending) :
πIt is a condition of stress where a bending moment is applied to a beam without the simultaneous presence of axial, shear, or torsional forces.
πPure bending occurs only under a constant bending moment (M) since the shear force (V), has to be equal to zero.
πIn reality, a state of pure bending does not practically exist, because such a state needs an absolutely weightless member.
πThe state of pure bending is an approximation made to derive formulas.
βοΈβοΈβοΈ
Assumptions:
β΄οΈThe material of the beam is homogeneous and isotropic.
β΄οΈThe value of Young's Modulus of Elasticity is same in tension and compression.
β΄οΈThe transverse sections which were plane before bending, remain plane after bending also.
β΄οΈThe beam is initially straight and all longitudinal filaments bend into circular arcs with a common centre of curvature.
β΄οΈThe radius of curvature is large as compared to the dimensions of the cross-section.
β΄οΈEach layer of the beam is free to expand or contract, independently of the layer, above or below it.
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π14
π°It is three-dimensional
homogeneous flattening of a body.
π°It is an example of irrotational strain in which body is elongated in one direction while being shortened perpendicularly.
π°For soft materials, such as rubber, a strain state of pure shear is often used for characterizing
hyperelastic & fracture mechanical
behaviour.
π°Pure shear is differentiated from simple shear in that pure shear involves no rigid body rotation.
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π5β€4
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RATIOS OF SHEAR STRESS -
Ratio
Shape (Ο)max / ( Ο )avg
Rectangle 1.5
Circle 1.33
Triangle 1.5
Diamond 1.125
Ratio
Shape (Ο)neutral axis / ( Ο ) avg
Rectangle 1.5
Circle 1.33
Triangle 1.33
Diamond 1
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π12β€3β€βπ₯1π―1
β Youngβs modulus or Modulus of elasticity (E) = Normal stress/ Normal strain
β Shear modulus or Modulus of Rigidity (G) = Shear stress/ Shear strain
β Bulk modulus (K) = Direct stress/ Volumetric strain
RELATIONSHIP BETWEEN E, G, and K -
β E = 2G(1 + 1/m) or E = 2G(1+Β΅)
β E = 3K (1-2/m) or E = 3K (1-2Β΅)
β E = 9KG/ (G + 3K)
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π3β€1
Number of total elastic constants (TEC) and independent elastic constants (IEC) based on material -
MATERIAL TEC IEC
Isotropic 4 2
Orthotropic 12 9
Anisotropic β 21
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π5
Shear force - It is algebraic sum of forces acting on beam at either left or right of considered section
Moment of force - It can be formulated as the product of force and the length of the line crossing over the point of support.
Couple - It is a moment that is generated of two forces having the same magnitude, acting in the opposite direction equidistant from the reaction point.
Torque - It is a moment having a tendency to to twist a body around its axis of rotation.
The point of Inflection - It can be defined as the point in the bending moment diagram where the bending moment is becomes β 0 β.
Point of contraflexure - Point at which the bending moment curve of the beam changes its sign.
Shear Span - Span having constant shear force value is termed as shear span.
Pure bending - when shear force is zero and value of bending moment is constant then it is called as pure bending.
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π₯SOM Very IMP One liners:
π΄1st derivative of deflection(β)gives slope(ΞΈ)
π΄2nd derivative of deflection(β) gives moment(M)
π΄ 3rd derivative of deflection(β) gives shear force(S)
π΄ 4th derivative of deflection(β) gives intensity of loading(W)
π΄Slope of bending moment diag. gives shear force
π΄Negative slope of shear force diag. gives loading intensity
#som
@macedhuleπ
π΄1st derivative of deflection(β)gives slope(ΞΈ)
π΄2nd derivative of deflection(β) gives moment(M)
π΄ 3rd derivative of deflection(β) gives shear force(S)
π΄ 4th derivative of deflection(β) gives intensity of loading(W)
π΄Slope of bending moment diag. gives shear force
π΄Negative slope of shear force diag. gives loading intensity
#som
@macedhule
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π12β€3
Pure bending:
( Theory of simple bending) :
πIt is a condition of stress where a bending moment is applied to a beam without the simultaneous presence of axial, shear, or torsional forces.
πPure bending occurs only under a constant bending moment (M) since the shear force (V), has to be equal to zero.
πIn reality, a state of pure bending does not practically exist, because such a state needs an absolutely weightless member.
πThe state of pure bending is an approximation made to derive formulas.
βοΈβοΈβοΈ
Assumptions:
β΄οΈThe material of the beam is homogeneous and isotropic.
β΄οΈThe value of Young's Modulus of Elasticity is same in tension and compression.
β΄οΈThe transverse sections which were plane before bending, remain plane after bending also.
β΄οΈThe beam is initially straight and all longitudinal filaments bend into circular arcs with a common centre of curvature.
β΄οΈThe radius of curvature is large as compared to the dimensions of the cross-section.
β΄οΈEach layer of the beam is free to expand or contract, independently of the layer, above or below it.
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( Theory of simple bending) :
πIt is a condition of stress where a bending moment is applied to a beam without the simultaneous presence of axial, shear, or torsional forces.
πPure bending occurs only under a constant bending moment (M) since the shear force (V), has to be equal to zero.
πIn reality, a state of pure bending does not practically exist, because such a state needs an absolutely weightless member.
πThe state of pure bending is an approximation made to derive formulas.
βοΈβοΈβοΈ
Assumptions:
β΄οΈThe material of the beam is homogeneous and isotropic.
β΄οΈThe value of Young's Modulus of Elasticity is same in tension and compression.
β΄οΈThe transverse sections which were plane before bending, remain plane after bending also.
β΄οΈThe beam is initially straight and all longitudinal filaments bend into circular arcs with a common centre of curvature.
β΄οΈThe radius of curvature is large as compared to the dimensions of the cross-section.
β΄οΈEach layer of the beam is free to expand or contract, independently of the layer, above or below it.
#som
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@macedhule
β€8π1