Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format: EGBC National Exam, 22-Mec-A2 “Kinematics and Dynamics of Machines”, May 2015 (source code 07-Mec-A2). Open-book, 3 hours; six questions of equal value (20 marks each), candidates answer any five. Part A — mechanisms and machine dynamics (Q1–Q4); Part B — mechanical vibration (Q5–Q6). All six are solved in full below.
Reference texts: R. L. Norton, Design of Machinery, 5th ed. (instant centres & mechanical advantage, cam design, four-bar force balancing, epicyclic trains); S. S. Rao, Mechanical Vibrations, 6th ed. (multi-DOF free vibration, modal analysis, impact response); J. E. Shigley & C. R. Mischke, Mechanical Engineering Design (epicyclic train-value cross-check).
Given. A six-bar linkage with three frame pivots. Reading the pin topology directly off the printed drawing, the chain is a Stephenson-type six-bar built on two ternary links:
crank 2 (the “Driver”): frame pivot O2 to pin A, driven at $\omega_2 = 100\ \text{rad/s}$ CW;
ternary link 3 (the lower shaded triangle): pins A, C and D;
binary rocker 4: frame pivot O4 (the upper ground bracket) to pin D — the bar that crosses link 6 in the drawing;
ternary link 5 (the upper shaded triangle): pin C, pin E and the free Tracer point;
output rocker 6: frame pivot O6 (the lower ground bracket) to pin E.
The mechanism is therefore two four-bars in cascade sharing the ternary link 3: loop 1 is O2–A–D–O4, and link 3 rigidly carries pin C into loop 2, C–E–O6. Joint coordinates measured from the printed figure of the 1:5 drawing (drawing units, $x$ right, $y$ up; 1 unit = 0.423 mm at full size):
Point
x
y
Joint / role
O2
126
372
frame pivot of crank 2 = I12
A
484
238
pin 2–3 = I23
C
1006
301
pin 3–5 = I35
D
1146
100
pin 3–4 = I34
O4
714
590
frame pivot of rocker 4 = I14 (upper bracket)
E
1060
538
pin 5–6 = I56
O6
720
423
frame pivot of output 6 = I16 (lower bracket)
Tracer
1522
304
free coupler point on link 5
Find. (i) the $n(n-1)/2 = 15$ instant centres, (ii) the mechanical advantage $\mathrm{MA}=\omega_{in}/\omega_{out}$, and (iii) $\omega_6$ (magnitude and sense).
[Figure not reproduced: The six-bar redrawn from the measured joint coordinates. Link 3 (A–C–D) and link 5 (C–E–Tracer) are ternary; rocker 4 runs from the upper bracket O 4 to pin D and crosses rocker 6, which runs from the lower bracket O 6 to pin E. The input–o. See the official exam paper.]
Approach. Establish the pin topology from the drawing first, locate the primary instant centres by inspection (pin joints and frame pivots), complete the set with Kennedy’s three-centre theorem, then use the common velocity of I26 for $\omega_6$ and the mechanical advantage; cross-check $\omega_6$ with a two-loop relative-velocity solution.
Fix the pin topology before anything else. The two ground brackets sit almost one above the other and the two bars leaving them cross, so it is easy to attach rocker 4 to the wrong pin. There is therefore no triple pin here: links 3 and 5 meet at C, links 3 and 4 meet at D, and $I_{45}$ must be found by Kennedy like any other secondary centre.
Count and classify the instant centres. With $n=6$ links, $$N = \frac{n(n-1)}{2} = \frac{6\cdot 5}{2} = 15.$$ Seven are read straight off the mechanism: the three frame pivots $I_{12}=O_2$, $I_{14}=O_4$, $I_{16}=O_6$, and the four pins $I_{23}=A$, $I_{34}=D$, $I_{35}=C$, $I_{56}=E$. The remaining eight follow from Kennedy’s three-centre theorem — for any three links the three shared centres are collinear, so each unknown centre is the intersection of two such lines.
The complete set of 15 centres (drawing units):
Centre
x
y
Located by
I12
126
372
O2 (inspection)
I13
1290
-64
Kennedy
I14
714
590
O4 (inspection)
I15
871
474
Kennedy
I16
720
423
O6 (inspection)
I23
484
238
A (inspection)
I24
23
334
Kennedy
I25
-1.07e+04
-1114
Kennedy
I26
-518
317
Kennedy
I34
1146
100
D (inspection)
I35
1006
301
C (inspection)
I36
983
199
Kennedy
I45
901
452
Kennedy
I46
722
356
Kennedy
I56
1060
538
E (inspection)
Output angular velocity from I26. Intersecting the Kennedy lines that share links 2 and 6 puts the input–output centre at $$I_{26} = (-518,\ 317)\ \text{drawing units},$$ which does lie on the line joining $I_{12}$ and $I_{16}$, as Kennedy requires. $I_{26}$ is the one point whose velocity is the same whether it is taken on link 2 or on link 6, so $$\omega_2\,\overline{I_{12}I_{26}} = \omega_6\,\overline{I_{16}I_{26}}.$$ With $\overline{I_{12}I_{26}} = 645.9$ and $\overline{I_{16}I_{26}} = 1242.1$ units, $$\omega_6 = \omega_2\,\frac{\overline{I_{12}I_{26}}}{\overline{I_{16}I_{26}}} = 100\times\frac{645.9}{1242.1} = \boxed{52.0\ \text{rad/s}}$$ The 1:5 scale cancels in the length ratio. $I_{26}$ lies outside the segment $I_{12}I_{16}$, so links 2 and 6 turn the same way: link 6 rotates clockwise, as the input does.
Mechanical advantage. Neglecting friction, input power equals output power, $T_2\omega_2 = T_6\omega_6$, so $$\mathrm{MA} = \frac{T_{out}}{T_{in}} = \frac{\omega_{in}}{\omega_{out}} = \frac{\omega_2}{\omega_6} = \frac{100}{52.0} = \boxed{1.92}$$ In this position the linkage multiplies torque about 1.9:1 (the output moves 1.9× slower than the input).
Independent relative-velocity check. Solving loop 1 (four-bar O2–A–D–O4) gives $\omega_3 = 44.4\ \text{rad/s}$ CCW and $\omega_4 = 14.8\ \text{rad/s}$ CW. Carrying $\omega_3$ across the rigid link 3 gives the velocity of pin C, and loop 2 (C–E–O6) then returns $\omega_5 = 93.6\ \text{rad/s}$ CW and $$\omega_6 = 52.0\ \text{rad/s}\ \text{CW},$$ identical to the instant-centre value — confirming both the topology and the measurements.
Quantity
Result
Instant centres
15 (7 by inspection, 8 by Kennedy)
Input–output centre I26
(−518, 317) drawing units
Output angular velocity $\omega_6$
52.0 rad/s (CW)
Mechanical advantage $\omega_2/\omega_6$
1.92
Check: The drawing carries no printed dimensions, so the joint coordinates were measured from the printed figure; only O2A, O4D and O6E are drawn as bars. The angular-velocity and mechanical-advantage results are ratios, hence insensitive to overall scale; a ±3 unit perturbation of every measured pin moves $\omega_6$ by only about ±2.4 rad/s and $\mathrm{MA}$ by about ±0.09, and the two independent methods agree to five figures. $I_{25}$ falls far off the page because the two Kennedy lines that fix it are nearly parallel in this position — geometrically legitimate, and it does not enter the answer.