Gerber beam: pin at 1 ($x=2$), rollers at 2 ($x=8$) and 3 ($x=14$), internal hinge at $x=10$, free ends at $x=0,16$.
Given. Supports at points 1 ($x=2$), 2 ($x=8$) and 3 ($x=14$); an internal hinge at $x=10$; free overhangs at both ends. Find. Three influence lines and their peak coefficients.
Approach. Place a unit load at position $p$, solve the determinate beam (using $M=0$ at the hinge as the fourth equation), and read the required response — the ordinate at each $p$ traces the influence line. Every influence line is piecewise-linear with break points at the supports, the hinge and the section.
(i) Moment at point 2. Zero while the load is anywhere between supports 1 and 2, it grows linearly to $-2.0$ when the load sits over the hinge ($x=10$), returns to zero at support 3, and reaches $+1.0$ at the free right end. Peak $|\eta|=\boxed{2.0\ \text{m}}$.
(ii) Moment at mid-span of 1–2 ($x=5$). A triangle peaking at $+1.5$ m under the section, negative ($-1.0$) over the overhangs and the hinge. Peak $|\eta|=\boxed{1.5\ \text{m}}$.
(iii) Shear just left of support 2. Rises to $-1.0$ as the load approaches the section from the span side and falls off over the rest of the beam. Peak $|\eta|=\boxed{1.0}$.
Cambered truss loaded on the bottom chord; the influence line for member $U_1L_3$ is drawn below.
Given. Six bottom joints at $4$ m spacing (span $20$ m); the diagonal $U_1L_3$; a three-axle group $18$–$18$–$8$ kN with $4$ m then $2$ m spacing. Find. IL ordinates and the maximum $U_1L_3$ force.
Ordinates. Placing a unit load successively at each bottom joint and solving for $U_1L_3$: $\eta_{L_1}=0,\ \eta_{L_2}=-\tfrac{7}{12}=-0.583,\ \eta_{L_3}=+0.500,\ \eta_{L_4}=+0.333,\ \eta_{L_5}=+0.167,\ \eta_{L_6}=0$; the line is linear between joints.
Position for maximum tension. Slide the group so the two 18 kN axles straddle the peak: $18$ kN at $L_3$ ($\eta=0.500$), $18$ kN at $L_4$ ($\eta=0.333$) and $8$ kN at $x=14$ ($\eta=0.250$).
Maximum force. $F_{\max}=18(0.500)+18(0.333)+8(0.250)=9+6+2=\boxed{17.0\ \text{kN (T)}}$. The largest compression the group can produce (over the negative lobe at $L_2$) is only $-10.5$ kN, so tension governs.
Quantity
Value
IL ordinates $\eta_{L_2},\eta_{L_3},\eta_{L_4},\eta_{L_5}$