22-Mec-A2 Kinematics and Dynamics of Machines · December 2016
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Reference texts (subject). R. L. Norton, Design of Machinery, 6th ed. (mechanisms, cams, gear trains); C. E. Wilson & J. P. Sadler, Kinematics and Dynamics of Machinery, 3rd ed.; Uicker, Pennock & Shigley, Theory of Machines and Mechanisms, 5th ed.; S. S. Rao, Mechanical Vibrations, 6th ed. (Part B). Balancing follows Norton Ch. 13; planetary trains Norton §9.7–9.9.
Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.
Given. Stage 1: sun $2$ ($N_2=18$), planet $3$, ring $4$ ($N_4=60$), carrier $c_1$. Stage 2: sun $5$ ($N_5=32$), planet $6$, ring $7$ ($N_7=86$), carrier $c_2$. The input shaft is the common carrier of both stages ($\omega_{c1}=\omega_{c2}=\omega_{in}=1800$ rpm), and sun 2 is rigidly joined to ring 7 on a floating sleeve ($\omega_2=\omega_7$); the output is sun 5. Brake $C$ holds ring 4; brake $D$ holds ring 7 — and therefore sun 2 with it.
Find. Planet teeth $N_3,N_6$; the maximum equally-spaced planet count in each stage; and the output speed with brake $C$ alone, and with brake $D$ alone.
[Figure not reproduced: Skeleton of the two-stage train traced from the section drawing: the input shaft is the common carrier of both stages, sun 2 and ring 7 are rigidly joined on a floating sleeve, and the output is sun 5. Brakes $C,D$ ground ring 4 / ring 7. See the official exam paper.]
Check (schematic interpretation). The section drawing carries no shaft labels, so the connectivity was traced from the printed figure itself. Three observations settle it. (1) The innermost line runs from the input arrow and its bearing to the right, and the only two members that reach down to it are the two planet-carrier arms, so the input shaft is the common carrier of both stages. (2) A second, slightly outer sleeve runs from the foot of the sun-2 column to the foot of the ring-7 drum, joining those two gears into one floating member. (3) A third, outermost sleeve with a free end carries ring 4 up to brake $C$. The drawn radii are self-consistent with this reading ($r_2+2r_3=r_4$ and $r_5+2r_6=r_7$ measured from the printed figure), and one brake then makes the output determinate in either mode. Both modes come out as speed increasers; that is what the drawn machine does, and the two brakes do give the "different speed ratios" the question asks for.
Approach. Coaxial (concentric) meshing requires the ring diameter to equal the sun plus two planets: $N_{\text{ring}}=N_{\text{sun}}+2N_{\text{planet}}$ (all gears share the pitch).
$$N_3=\frac{N_4-N_2}{2}=\frac{60-18}{2}=\boxed{21},\qquad N_6=\frac{N_7-N_5}{2}=\frac{86-32}{2}=\boxed{27}.$$
Two conditions must hold together: the assembly (equal-spacing) condition requires $(N_{\text{sun}}+N_{\text{ring}})/n_p$ to be an integer, and the adjacent-planet clearance requires $\sin(\pi/n_p)>(N_{\text{planet}}+2)/(N_{\text{sun}}+N_{\text{planet}})$ (full-depth addendum).
Approach. Each stage obeys the planetary relation $N_s\omega_s+N_r\omega_r=(N_s+N_r)\omega_c$. Both carriers are on the input shaft, so $\omega_{c1}=\omega_{c2}=1800$ rpm, and the single floating sleeve gives one coupling unknown $Z\equiv\omega_2=\omega_7$:
$$\underbrace{18\,Z+60\,\omega_4=78(1800)}_{\text{stage 1}},\qquad \underbrace{32\,\omega_5+86\,Z=118(1800)}_{\text{stage 2}}.$$
| Quantity | Value |
|---|---|
| (i) Planet teeth $N_3$ / $N_6$ | 21 / 27 |
| (ii) Max equally-spaced planets, stage 1 / stage 2 | 3 / 2 |
| (iii) Output with brake $C$ | −14,325 rpm (reversed; 7.96:1 step-up) |
| (iv) Output with brake $D$ | +6637.5 rpm (same sense; 3.69:1 step-up) |