IntermediateFrameConnectionsMoment releasePortal

Moment vs shear connections — what a release actually costs

Change the rafter’s connections from moment to shear and the frame stops being a frame. The rafter reverts to a simply supported beam carrying the full , and the columns carry no moment at all — one switch, and an exact hand answer appears.

Figure 1.A fixed-base portal with both rafter ends released — shear connections, marked by the open circles.
Given
Span
6 m
Height
4 m
10 kN/mon the rafter
Rafter ends
RELEASEDshear connections
Bases
fixedpinned would be a mechanism
1

Part 1 — Build it, then release the rafter

One switch in the toolbar changes what the structure IS.

Build the fixed-base portal exactly as before:

N 0,0 N 0,4 N 6,4 N 6,0 M 1 2 M 2 3 M 4 3 S 1 F S 4 F L 2 -10

Now release the rafter’s ends. Select the rafter, then set its Connection to Shear — or right-click either end and switch that end alone. A released end carries shear and axial force but no moment, and the drawing marks it with a small open circle just inside the member end.

That single change is the whole experiment. Everything else — geometry, section, load, supports — is identical to the rigid version, so every difference below is caused by the connection.

Figure 2.The portal with both rafter ends released — note the open circles marking the shear connections.
2

Part 2, step 1 — Why the bases had to be fixed

The release you cannot make.

Try this with pinned bases instead and the solver refuses to run, reporting that the frame is a mechanism. It is right. With pinned feet and both rafter ends released, every column end is a pin — nothing anywhere resists the frame simply folding sideways.

That refusal is worth dwelling on. A moment connection is not a refinement you can delete wherever you like: in many frames it is the only thing making the structure stable. The bases are fixed here so that the frame stands up and the cost of the release can actually be measured.

3

Part 2, step 2 — The frame action disappears

Exactly wL²/8 — the release turns the rafter back into a beam.

With both ends released, the rafter can no longer hand moment to the columns. It carries its load exactly as a simply supported beam would:

The solver returns 45 kN·m — the textbook value to the decimal, in a frame that is otherwise indeterminate.

And the columns now carry 0 kN·m of moment. Zero. They have become props: pure axial members holding the beam up.

Compare the rigid version: rafter 22.55 kN·m, columns 22.45 kN·m. The moment connections were sharing the work. Release them and the rafter absorbs everything the columns were helping with.

Figure 3.The released frame. The rafter carries the full simply-supported moment; the columns carry axial load only.

Hand calculation vs solver

A rare case where the indeterminate frame gives an exact hand answer.

Verified — hand calculation vs the solver, to round-off
QuantityBy handStructureCalcs
Total vertical reactionwL = 60 kN60 kN
Rafter peak moment — RELEASEDwL²/8 = 45 kN·m45 kN·m
Column moment — RELEASED0 (pure axial)0 kN·m
Rafter peak moment — rigid twinindeterminate22.55 kN·m
Column moment — rigid twinindeterminate22.45 kN·m

Every value was worked by hand with the classical method, then checked against this site’s solver — the same engine the Try it button opens. This agreement is re-run automatically on every build.

Now make it yours

Open this exact model in the calculator — then change a load, drag a support, and watch every diagram update in real time. The best way to build intuition is to break it and see what happens.

Take it with you

Export this worked example as a PDF, or download it as a .screport and open it in the Report Builder — the model travels inside the file, so you can reconstruct it, re-solve, and build your own report from it.

Verifying your link…