How much of the load is “Distributed across ” the central section?
One assumes “all of it”. The initial post is clear – the entire length of the beam is not loaded, only some of its length.
Details concerning support conditions are perhaps irrelevant at this stage.
It would be useful, instead of referring to 800 pages plus of Machinery’s Handbook, to actually go and look at a copy (online ones are available) and cite a specific page where the actual question can be answered.
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If a person wants a conceptual understanding, the easiest place to start is a point load midspan of a simply-supported solid rectangular section. For that, the midspan deflection formula is:
delta = PL^3/48EI
where P is the load, L is the length, E Young’s modulus, I second moment of area. Side note that for a rectangualr section I = bd^3/12 where b is width and d is height.
This tells us a lot, all of which is intuitive on reflection: the deflection is directly proprtional to the load P. The deflection varies with the cube of the span length (so twice the span gives eight times the deflection). The deflection is inversely proportional to the Young’s modulus – use a material twice as stiff for half the deflection. The deflection is inversely proportional to the I-value, so double the I value for half the deflection.
The I value, second moment of area, reflects how the material of the section is distributed relative to the bending (neutral) axis of the section. With the rectangular section, double the width, double the I value. Double the depth, the I value increases eightfold. That is why an I-beam is the shape it is – it puts as much of the material in the flanges, as far away from mid-depth as possible.
Other loading cases and support conditions are just more complex cases of this most basic example. The important take away is how the four factors (load, span, material stiffness, material distribution) affect the deflection.