Question 3 of 9: Castigliano's theorem — deflection at an internal hinge
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams – May 2019,
07-Str-A4 Advanced Structural Analysis. Three hours, closed book (an approved Casio or
Sharp calculator is the only aid). Nine questions: #1 and #2 are compulsory,
then any two of #3, #4, #5 and any two of #6, #7, #8, #9 —
six questions constitute a complete paper and total 100 marks. Marks are printed in the left
margin (9, 11, 18, 18, 18, 22, 22, 22, 22). All nine questions are solved here,
because the set is a study resource rather than a three-hour sitting.
Reference texts. R. C. Hibbeler, Structural Analysis, 10th ed.
(slope-deflection, moment distribution, Castigliano and the force method);
A. Kassimali, Structural Analysis, 6th ed. (degrees of freedom, influence of support
settlement and lack of fit); J. C. McCormac, Structural Analysis: Using Classical and
Matrix Methods, 5th ed. (matrix formulation of the stiffness equations);
CSA S16:19 Design of Steel Structures and CSA A23.3:19 Design of Concrete
Structures for the Canadian design context in which these analyses are used.
Question 3: Castigliano's theorem — deflection at an internal hinge (18 marks)
Given. A beam ABCD built in at A and carried on a roller at D, with
an internal hinge at C. Each bay is 3 m long. A uniformly distributed load of 8 kN/m acts over
AB and a second uniformly distributed load of 8 kN/m acts over CD; the middle bay BC is
unloaded.
Given data
Symbol
Value
Meaning
$EI$
$3.0 \times 10^{4}$ kN·m$^{2}$
flexural rigidity, constant throughout
$w$
8 kN/m
intensity of both distributed loads
AB = BC = CD
3 m each
bay lengths, 9 m overall
A
built in
three reaction components
C
internal hinge
bending moment identically zero
D
roller
vertical reaction only
Find. The vertical deflection of point C, the hinge, in millimetres,
together with its direction.
Question 3: beam built in at A, internal hinge at C, roller at D; 8 kN/m over AB and over CD.
Approach. The hinge makes the structure determinate, so split it
there: CD is a simply supported span whose reaction at the hinge is a known force on the
remaining cantilever AC, and Castigliano's first theorem is then applied to that cantilever
alone with a dummy force $Q$ at C.
Check that the structure is determinate. The reactions are three at
A and one at D, four in all, against three equations of equilibrium plus the condition
$M_C = 0$ supplied by the hinge. Four equations for four unknowns, so no redundant exists and
the internal forces follow from statics alone — which is what makes a single Castigliano
integral sufficient.
Isolate span CD and find the force it hands to the hinge. CD spans
3 m between the hinge at C and the roller at D and carries 8 kN/m, with zero moment at both
ends, so it behaves as a simply supported span. Taking moments about C,
$$R_D = \frac{w\,a^{2}/2}{a} = \frac{w\,a}{2} = \frac{8 \times 3}{2} = \boxed{12\ \text{kN}}$$
and by vertical equilibrium the hinge delivers the other half, $V_C = 8(3) - 12 = 12$ kN,
downwards on the cantilever AC.
Reduce the problem to a cantilever. Everything to the right of the
hinge is now replaced by that 12 kN tip force, so AC is a 6 m cantilever built in at A, carrying
8 kN/m over its first 3 m (the AB bay) and a 12 kN point load at its tip. Its base reactions
follow immediately:
$$R_A = 8(3) + 12 = 36\ \text{kN}, \qquad
M_A = 8(3)(1.5) + 12(6) = 36 + 72 = \boxed{108\ \text{kN}\cdot\text{m}}$$
(hogging), which will serve later as an arithmetic check.
Introduce the dummy load and write the moment function. Add a
vertical force $Q$ at C in the direction of the required deflection and measure $s$ from C
towards A. Only the tip forces act over the first 3 m; beyond that the UDL enters:
$$M(s) = -(12 + Q)\,s \qquad (0 \le s \le 3)$$
$$M(s) = -(12 + Q)\,s - \tfrac{1}{2}w\,(s-3)^{2} \qquad (3 \le s \le 6)$$
Note that span CD stores strain energy but its moments do not contain $Q$: a force applied
at the hinge is carried straight into the cantilever and does not load the simply
supported span, so that segment contributes nothing to the derivative.
Apply Castigliano's first theorem. With
$\partial M/\partial Q = -s$ throughout and $Q$ set to zero after differentiating,
$$\Delta_C = \frac{\partial U}{\partial Q}\bigg|_{Q=0}
= \frac{1}{EI}\int_{0}^{6} M\,\frac{\partial M}{\partial Q}\,ds
= \frac{1}{EI}\left[\int_{0}^{6} 12s\cdot s\,ds
+ \int_{3}^{6} 4(s-3)^{2}\,s\,ds\right]$$
Both integrands are positive, which already tells us the deflection is downwards, in the
direction assumed for $Q$.
Evaluate the two integrals. The tip-load term is the familiar
cantilever result:
$$\int_{0}^{6} 12s^{2}\,ds = 12\,\frac{6^{3}}{3} = 864
\qquad\Longleftrightarrow\qquad \frac{P L^{3}}{3} = \frac{12(216)}{3} = 864$$
For the distributed term substitute $u = s - 3$:
$$\int_{3}^{6} 4(s-3)^{2}s\,ds = 4\int_{0}^{3}u^{2}(u+3)\,du
= 4\left[\frac{u^{4}}{4} + u^{3}\right]_{0}^{3} = 4(20.25 + 27) = 189$$
The same figure follows from the standard partial-UDL cantilever formula
$w a^{3}(4L - a)/24 = 8(27)(24 - 3)/24 = 189$.
Add the two contributions and put in the numbers.
$$\Delta_C = \frac{864 + 189}{EI} = \frac{1053}{EI}
= \frac{1053}{3.0 \times 10^{4}} = 0.0351\ \text{m}$$
$$\boxed{\Delta_C = 35.1\ \text{mm downwards}}$$
The tip load supplies 28.8 mm of that and the partial UDL only 6.3 mm, because the distributed
load sits close to the built-in end where the unit-load lever arm is small.