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Direct integration of a beam

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Through Integral, Free body diagram and Steel

For a beam with an applied weight w(x), taking downward to be positive, the internal shear force is given by taking the negative integral of the weight:

V(x)=−∫w(x)dx

The internal moment M(x) is the integral of the internal shear:

M(x)=∫V(x)dx = −∫[∫w(x)dx]dx

The angle of rotation from the horizontal, θ, is the integral of the internal moment divided by the product of the Young's modulus and the area moment of inertia:

θ(x)=1EI∫M(x)dx

Integrating the angle of rotation obtains the vertical displacement ν:

ν(x)=∫θ(x)dx

Integrating

Each time an integration is carried out, a constant of integration needs to be obtained. These constants are determined by using either the forces at supports, or at free ends.

For internal shear and moment, the constants can be found by analyzing the beam's free body diagram.
For rotation and displacement, the constants are found using conditions dependent on the type of supports. For a cantilever beam, the fixed support has zero rotation and zero displacement. For a beam supported by a pin and roller, both the supports have zero displacement.

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