Transformation Laplace Problem 3: Evaluate L{e-3 t}
Transformation Laplace Problem 4: Evaluate L{sin 2 t}
Transformation Laplace Problem 2:
Inverse Transform
Linear Transform
Inverse Transform Problem 1:
Inverse Transform Problem 2:
Inverse Transform Problem 3:
Applications Deflection of Beams Axis of symmetry Deflection of curve Beam is assumed as a homogeneous, and has uniform cross sections along its length Deflection curve can be derived from differential equation based on elasticity concept.
Applications Deflection of Beams 0 L x y(x) y Elasticity theory: bending moment M(x) at a point x along the beam is related to the load per unit length w(x)
Applications Deflection of Beams 0 y L x y(x)
Applications Deflection of Beams l 0 y L x l y(x) l l y(0) = 0 at embedded end. y’(0) = 0 (deflection curve is tangent to the x-axis at embedded end) y”(L) = 0, bending moment at free end is zer 0. y”’(L) = 0, shear force is zero at a free end. EIy’’’ = d. M/dx is the shear force.
Applications Determining deflection of a Beam using Laplace Transform w 0 Wall x L y A beam of length L is embedded at both ends. In this case the deflection y(x) must satisfy:
Applications Determining deflection of a Beam using Laplace Transform
Applications Determining deflection of a Beam using Laplace Transform