Tutorial 4 Q5: opposite reactions and equal moment sharing
Open “Animation lab” beside a teaching step for a visual explanation or a walkthrough of its original expressions. Models are illustrative; source answers remain unchanged.
Need a simpler picture? Open “Simple explanation” beside a difficult step. These optional notes do not replace the full solution.
Check UC S355 below a simple-construction floor joint. Effective length ; actual height . Upper/lower column stiffnesses are equal. All shown loads are first-order ultimate values: central ; Fₓ₁150 at left, Fₓ₂100 at right; Fᵧ₁180 at above, Fᵧ₂300 at below in plan. Amplification .
Original source: LectureNotes/Ch 4_Column.pdf — p. 41. Values tagged given are in the question or diagram; lookup values come from a named table; calculated values follow from the working; assumptions are stated explicitly.
Read the diagram and collect the data
Lookup: Data File p.11, exact row UC. Read the dimensions/local ratios table and the properties table separately. The axis crosses the web horizontally; passes vertically through its centre in the table sketch.
| Property | Value and units |
|---|---|
| Flange/web/root-to-root web depth | 、、。 |
| Local slenderness | 、。 |
| Radii (converted from ) | ;。 |
| Area | 。 |
| Elastic moduli | ;。 |
| Plastic moduli | ;。 |
| LTB parameters | , ; both dimensionless |
Before calculating: recognition and strategy
Resolve two separate balances at the floor joint: the column below carries all downward force, while net moment is shared equally between upper and lower columns by the given equal stiffness. Use effective for compression and actual for the special simple-construction LTB expression.
1. Sum compression and opposing moments
The central is described as axial force above, including self-weight; do not add self-weight again. The lower segment takes the full . The upper segment is not assigned half of that load.
Animation labFollow the floor load in 3D
Supplement to the original lesson. Enable JavaScript to play, step through calculations and rotate 3D models. The following explanation remains readable offline.
- The floor carries pressure in . The highlighted strip belongs to one secondary beam.
- Multiply pressure by tributary width: . The illustration uses .
- A primary beam receives the secondary beam reaction at their connection, not a new full-span UDL.
- Trace reactions down to columns and foundations. Count each loaded area once.
3. Section interaction
At a cross section, compression and bending share the material. Use amplified moments and capped plastic resistances. The total must not exceed ; all terms below are dimensionless.
Animation labA strong slice can belong to an unstable member
Supplement to the original lesson. Enable JavaScript to play, step through calculations and rotate 3D models. The following explanation remains readable offline.
- Combine axial compression and the two bending demands using the specified section resistances.
- The whole member adds effective-length and buckling-curve effects.
- This uses its own moment factor and bending resistance; it is not a copy of the section check.
- Elastic, plastic and buckling resistances are not interchangeable. Read the three original expressions and their first-order/amplified moments.
4. Flexural member interaction using
Simple explanation: The column needs more than one pass
A slice can be strong while the whole member still buckles.
- Check cross-section compression plus bending.
- Then check the separate member-buckling expressions.
- Keep each moment, factor and resistance in its specified expression.
Remember: The three checks do not share interchangeable denominators.
Table 8.7: hot-rolled H-section (UC), maximum thickness , about the axis use curve , about the axis use curve . Use the Data File p.8 column. The two axes use different curves, so slenderness alone cannot identify the governing axis.
Member interaction uses elastic moment denominators pᵧZ, even when the cross-section check used plastic moduli. Use amplified moments here.
Animation labA strong slice can belong to an unstable member
Supplement to the original lesson. Enable JavaScript to play, step through calculations and rotate 3D models. The following explanation remains readable offline.
- Combine axial compression and the two bending demands using the specified section resistances.
- The whole member adds effective-length and buckling-curve effects.
- This uses its own moment factor and bending resistance; it is not a copy of the section check.
- Elastic, plastic and buckling resistances are not interchangeable. Read the three original expressions and their first-order/amplified moments.
5. Simple-construction LTB using actual
Simple explanation: A beam can escape sideways
The compressed flange can move sideways while the section twists.
- Divide the beam at effective lateral restraints.
- Use each segment’s effective length to obtain its buckling resistance.
- Compare that resistance with the segment’s equivalent moment demand.
Remember: A section bending check alone does not check lateral-torsional buckling.
Simple-construction special rule: use actual storey length in 0.5L/rᵧ; the axial effective length is a different quantity.
Read Data File p.5 Table 8.3a, pᵧ345 column:
Course Eq.8.81 uses first-order minor-axis moment in its last term. Mᴸᵀ is the specified amplified major-axis value; do not amplify it twice. The axial denominator is .
; , ; , . . Ratios: section , flexural buckling , axial force/LTB . At least one required ratio exceeds , so the column fails.
Animation labA strong slice can belong to an unstable member
Supplement to the original lesson. Enable JavaScript to play, step through calculations and rotate 3D models. The following explanation remains readable offline.
- Combine axial compression and the two bending demands using the specified section resistances.
- The whole member adds effective-length and buckling-curve effects.
- This uses its own moment factor and bending resistance; it is not a copy of the section check.
- Elastic, plastic and buckling resistances are not interchangeable. Read the three original expressions and their first-order/amplified moments.
Compact exam answer
Lower F1,930 kN. Joint Mx 39.6/My 22 kNm; half-shares /; amplified /12.65. LE5,100 mm for axial buckling; L6,000 mm for λᴸᵀ=0.5L/rᵧ. All .
; , ; , . . Ratios: section , flexural buckling , axial force/LTB . At least one required ratio exceeds , so the column fails.
Mistakes to avoid
- Do not use for a flange thicker than .
- Do not substitute plastic moduli in the member elastic denominators.
- Do not amplify an already amplified Mᴸᵀ twice.
- Do not treat an axial resistance pass as proof of combined-load adequacy.
- Do not halve the axial force when halving joint moment.
- Do not add magnitudes of opposite-side eccentric moments.
- Do not use in the actual-height LTB rule.
Procedure for an unfamiliar variant
- Identify construction type, axis, actual length and effective length.
- Read thickness, grade and the exact UC row. Classify before using plastic moduli.
- Sum vertical forces and derive signed eccentric moments; share moments only when the joint has two columns.
- Apply specified amplification once. Check the capped section interaction.
- Select curves / for these rolled H sections, interpolate both strengths and check flexural interaction with elastic moduli.
- Use the appropriate simple/continuous LTB slenderness rule and the course first-order minor-axis term.
- Report every utilisation and let any failed check govern.
Independent self-check
Try it yourself. Invented variant: the lower column has twice the upper column’s stiffness, with all loads unchanged. Find its first-order moments.
Reveal answer and reasoning
Lower fraction=. ; . Amplified moments and . Axial load remains . All interactions must be recalculated; the stiffer lower column attracts more moment.
Animation labEccentric reactions and stiffness sharing
Supplement to the original lesson. Enable JavaScript to play, step through calculations and rotate 3D models. The following explanation remains readable offline.
- A beam reaction can act away from the column centre even at a nominally pinned beam connection.
- . Opposing reactions can cancel part of the signed moment, while both still add compression.
- The course simple model distributes the joint moment in proportion to of the columns above and below.
- Equal relevant stiffness gives half each. A roof joint with no upper column is a different case.