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#1
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| When calculating transverse frames what would be ... When calculating transverse frames what would be the unsupported length (GL rules) when one has a strong deck beam inside from an accomodation deck? ![]() |
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#2
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| A "A". Regards |
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#3
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#4
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| Quote:
![]() Seriously now ... wouldn't a beam as strong as a frame count as adequate support? If it doesn't that means the inner deck structure doesn't participate in the stiffening of the structure at all? |
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#5
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| I can tell you as an experienced professional engineer, that if the floor is structurally tied to the frame, I would instantly say "A" is the unsupported length. Tobbe is correct, any other answer is incorrect. Also note that the frame has continuous lateral support, so laterally the frame has "zero" unsupported length in lateral direction if the skin or planking is continuously attached to the frame. this affects the size limits of the frame (it can be lighter since it is restrained from buckling laterally). |
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#6
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| Not familiar with GL rules but here are from LR and ABS which I posted sometime ago. Seems your frame angle is greater than 150 degrees. |
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#7
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| I don't think most classification societies would consider a lower deck beam "floating" between port and starboard transverse frames as adequate support for the same frame that is supporting the beam. However, if the lower deck beam were effectively tied to the floor (the structural transverse floor at the keel) with pillars and/or brackets, as in double bottom construction, then it may provide adequate support for the transverse frame and the span may be reduced to "A". |
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#8
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| I checked the GL rules as downloaded from the link provided by MikeJohns. You may search it if here if you don't have it. "Chapter 1 section 3 C. Unsupported Span 1. Stiffeners, frames The unsupported span is the true length of the stiffeners between two supporting girders or else their length including end attachments (brackets)." And "I - Part 1 GL 2011 Section 9 Framing System" which shows there is a distinction between bottom transverse and side transverse. However, your illustration shows a section which seems to be a (forward/aft) end of the vessel. Is this a discontinous floor or a double bottom? I interpret it as one is a raised floor (or horizontal bulkhead). This being the case, the unsupported span will be "A" for the aft part and "B" for the forward part assuming both floor (or 'tween deck) is bracketed as Paul and Petros has correctly interpreted. Can you post a profile of the floor? |
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#9
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| Hello, A little question about the sketch given by RXComposite : il seems to me that the L.R. and the ABS rules have different interpretation on the "middle point" for a curved traverse frame for calculating the local pressure. Is it true that : for LR, the midpoint take in account the curvature on the frame ; for ABS, the midpoint is simply the mid-length of the chord between the gunwale and the end of the floor. In the first case, the pressure is generaly bottom pressure, et in the second, this is the side pressure ? Thank you in advance Jacques |
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#10
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| Jaques, In the original post of the illustration, it was to show that the distinction between the bottom transverse and the side transverse vanishes when the angle is equal to or greater than 150 degrees. It simply becomes one single transverse. It was also to emphasize that curved or chined, the rule is the same. So for angles less than 150 degrees, two calculations are needed. One for bottom transverse, and one for side transverse. As for the curvature, a factor is added to the calculation to account for the increased stiffness of the structure brought about by the curve. The determination of midpoint as shown by the rules is important because; 1. It determines where the additional stiffeners will be located. 2. It determines the point where the pressure will be applied for calculations where midpoint has the greatest moment. 3. It determines the point from the y axis the amount of pressure that will be exerted. That is pressure increasing as the point gets deeper. GL measures this from the baseline, LR measures this from the waterline. No. 3 is simplifying it a bit. Dynamic pressure is used (that is when the boat is moving). When the boat is moving, a bow wave (and stern wave) is created, raising the static waterline and increases the height of pressure. which explains why the "V" in the fore end or aft end is treated as one member. Using the pressure formula, try plotting the pressure along the length of the boat and at different depths. you will find that the distribution is greater on the fore end and aft end of the boat (ship) and diminishes towards the midship. |
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#11
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| Thank you for your answer. In fact, I thinked to a sailboat : as the curvature is "soft", it is difficult to slit the frame in two part : bottom et side. The ABS ORY rules do not take account of the curvature factor, but it is the case for ISO rules ... And it seems to me that the ISO use the same method of L.R. ... |
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#12
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| Quote:
For the curvature, it is taken into account. See the rule on "c", the correction factor for curved plating. For ABS ORY, it is not to be less than 0.70 and a table is given, but for steel vessel it is simply stated c=0.915. See attached rules on plating. My rulebook is old so there might be some changes. |
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#13
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| Thank you very much for your answer. But it seems to me that ABS ORY take in account the curvature factor only for the plating, but not for the transverse frame ... But maybe my interpretation is wrong ? |
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#14
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| Quote:
if loads are symmetrical, like in submerged submarine, span would be A, provided that this cross tie is safe for buckling. ____________________ To play safe, I would assume span B.
__________________ All the stresses in my designs are 95% of permissible. |
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#15
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| Quote:
The mentioned rules (from what I can see) make no distinction between side transverse and bottom transverse, unless you're referring to transverse frames and bottom floors. Quote:
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