This is an interesting discussion and something I've pondered before but never really investigated further until now.
In general, I agree with Mike Mike's method above.
I think the most theoretically correct approach would be:
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[li]For a beam in biaxial bending with moments Mx and My about the beam's x and y (strong and weak) axes, find the angle of the neutral axis which results in moments having the same ratio as Mx and My, or which has the same resultant angle as the resultant moment Mxy. For example if Mx and My both happened to be equal, then the resultant moment, Mxy = 1.414*Mx and the angle of Mxy is 45 degrees. Be aware that this angle is most likely
not equal to the angle of the neutral axis. In the case that the section is square (double symmetric section) it will be equal, but for other cases, like a slender section (2x8 for ex.) it won't.[/li]
[li]Next, given the neutral axis angle found above, solve for the max shear stress. This stress occurs at the neutral axis (mid-depth of the member). This can be solved using the equation: fv = VQ/Ib. The values Q and I need to be solved accounting for the neutral axis angle.[/li]
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I investigated both a 2x8 and 8x8 beam in biaxial bending and shear:
[URL unfurl="true"]https://res.cloudinary.com/engineering-com/image/upload/v1699550010/tips/Biaxial_Bending_and_Shear_Investigation_-_2x8_and_8x8_-_2023-11-09_sxf03s.pdf[/url]
To attempt to answer the OP's original question:
Suppose you were to load a 2x8 beam equally about both x and y axes, resulting in moments, Mx and My, of the same magnitude with the resultant moment, Mxy, at a 45 degree angle. Since the moments are equal, the section moduli, Sx and Sy, are also equal. From the 2x8 graph above, the point where Sx and Sy are equal (and intersect) is roughly at a neutral axis angle of 87 degrees (note that this is not at 45 degrees due to the slender section). Now, if the corresponding shear forces, Vx and Vy also happened to be equal, then the resultant shear force, Vxy, would be 1.414Vx. If you were to look at each shear force independently, you would find (see the chart) that fx_max = 0.138Vx and fy_max = 0.138Vx. You would also find that fxy_max = 0.132(1.414Vx) = 0.187Vx.
So, in this particular case, the resultant shear force, Vxy, produces a greater shear stress than the individual components of that force, Vx and Vy.
Perhaps the codes have overlooked this. Although, I think a slender member (like a 2x8) is unlikely to be loaded equally in both the strong and weak directions anyway, and even if it was, it would likely fail in bending first. There probably aren't many likely scenarios where the shear failure would control over a bending failure. Perhaps a large concentrated load applied near a support would be one.
For the 8x8 beam above, it's interesting to note that if the same loading scenario is investigated as for the 2x8, it's found that
the resultant shear force, Vxy, does not produce a greater shear stress than the individual components of that force, Vx and Vy. The difference here is that the 8x8 section is not slender, and in fact, at a 45 degree angle, the max shear stress is only 2/3 of the max in either of the orthogonal directions.
It can be observed that for a rectangular section, with width b and depth d:
[ol 1]
[li]If the neutral axis is oriented perpendicular or parallel to the sides, fmax = 1.5 * V / bd[/li]
[li]If the neutral axis is oriented passing through the diagonal, fmax = 1.0 * V / bd[/li]
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In the graphs above, at the angles where the neutral axis passes through the member diagonal, the term that I refer to as the geometry/shape factor (fmax*A/V) is equal to 1.
Finally, as a conservative approach, I think it's reasonable to calculate the resultant shear force, Vxy, from the individual components, Vx and Vy, and then, assuming a rectangular section, calculate the max. shear stress as fmax = 1.5 * V / bd. As discussed above, using this approach could be conservative by 50 percent.