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22-Mec-A2 Kinematics and Dynamics of Machines · May 2018

Question 4 of 7: Compound planetary gear train with two ring brakes

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Reference texts (subject). R. L. Norton, Design of Machinery, 6th ed. (mobility Ch. 2, position/velocity Ch. 4–6, cams Ch. 8, epicyclic trains §9.6–9.9, balancing Ch. 13); Uicker, Pennock & Shigley, Theory of Machines and Mechanisms, 5th ed.; C. E. Wilson & J. P. Sadler, Kinematics and Dynamics of Machinery, 3rd ed.; S. S. Rao, Mechanical Vibrations, 6th ed. (Part B: single-DOF transient Ch. 2–4, two-DOF Ch. 5).

Open-book, 3 hours. Question 1 (40 marks) is compulsory; candidates then choose three of Q2–Q5 (Part A) and one of Q6–Q7 (Part B). Every question and sub-part is solved in full below.

Question 4: Compound planetary gear train with two ring brakes (20 marks)

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. Two coaxial simple-planetary stages on a common carrier. Stage 1: sun $B$ (input, $N_B=60$), planet $C$ ($N_C=31$), ring $D$ (held by its brake). Stage 2: sun $F$ (output, $N_F=25$), planet $G$ ($N_G=48$), ring $H$ (held). Both rings grounded; carrier free and common. $\omega_{in}=1450$ rpm CCW.

Find. $\omega_{out}$ (sense and magnitude).

winwoutB (sun 60)C (31)ring D (122) - brakeF (sun 25)G (48)ring H (121) - brakecommon carrier (free)
Compound planetary: input sun $B$ and output sun $F$ on the common axis, rings $D$ and $H$ grounded by friction pads, planets $C$ and $G$ on one free common carrier. With equal module, $N_D=N_B+2N_C=122$ and $N_H=N_F+2N_G=121$.

Approach. With equal module the ring teeth follow from the coaxial (radii-add) condition, $N_{\text{ring}}=N_{\text{sun}}+2N_{\text{planet}}$. For each stage use the fixed-carrier train value $e=-N_{\text{sun}}/N_{\text{ring}}$ in the epicyclic equation $(\omega_{\text{ring}}-\omega_c)/(\omega_{\text{sun}}-\omega_c)=e$. The common carrier speed links the two stages.

  1. Ring tooth counts. Equal module ⇒ pitch radius $\propto$ teeth, and ring $=$ sun $+$ 2 planet: $$N_D=N_B+2N_C=60+2(31)=122,\qquad N_H=N_F+2N_G=25+2(48)=121.$$
  2. Stage 1: carrier speed from the fixed ring $D$. Train value sun→planet→ring $e_1=-N_B/N_D$. With $\omega_D=0$: $$\frac{0-\omega_c}{\omega_B-\omega_c}=-\frac{N_B}{N_D}\;\Rightarrow\;\omega_c=\omega_B\,\frac{N_B}{N_B+N_D}=1450\cdot\frac{60}{182}=\boxed{478.0\ \text{rpm (CCW)}}.$$
  3. Stage 2: output sun $F$ from the same carrier and fixed ring $H$. $$\frac{0-\omega_c}{\omega_F-\omega_c}=-\frac{N_F}{N_H}\;\Rightarrow\;\omega_F=\omega_c\,\frac{N_F+N_H}{N_F}=478.0\cdot\frac{146}{25}.$$
  4. Combine. $$\omega_{out}=\omega_F=1450\cdot\frac{N_B}{N_B+N_D}\cdot\frac{N_F+N_H}{N_F}=1450\cdot\frac{60}{182}\cdot\frac{146}{25}=\boxed{2.79\times10^{3}\ \text{rpm}}.$$

Both stages preserve sense (a fixed-ring planetary turns its carrier and its sun the same way), so the output is CCW, the same sense as the input. The device is a step-up: the reduction sun $B\!\to$ carrier ($\times0.330$) is over-run by the amplification carrier $\to$ sun $F$ ($\times5.84$), netting $\omega_{out}/\omega_{in}=1.93$.

Check: the exam schematic is a bare section skeleton and does not print $N_D,N_H$; they are inferred from the equal-module coaxial condition ($N_{\text{ring}}=N_{\text{sun}}+2N_{\text{planet}}$), and $B,F$ are read as the on-axis suns (input/output shafts) with $D,H$ the braked rings. If instead each stage’s output were taken at its carrier, the train would be a step-down ($\approx82$ rpm); the sun-to-sun reading used here matches the input/output shafts drawn on the common axis.

QuantityValue
Ring teeth $N_D,\ N_H$$122,\ 121$
Common carrier speed $\omega_c$$478\ \text{rpm}$ (CCW)
Output speed $\omega_{out}$$\approx 2792\ \text{rpm}$, CCW (same sense as input)