Unit 4: Theory of Machines – Comprehensive Short Notes
(Aligned with RGPV Past Papers: Jun 2025, Dec 2024, Jun 2024, Jun 2023, Nov 2023, Jun 2022)
1. Fundamental Concepts
Mechanisms vs. Machines
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Mechanism: A set of links connected by joints to transmit motion/force. Focuses on kinematics (motion only).
Example: Slider-crank mechanism in an engine.
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Machine: A mechanism + additional elements (like frame, fasteners) to perform work with energy conversion.
Example: Complete engine assembly.
[!TIP]
Exam Key: Mechanism = motion transformer; Machine = work producer.
Degree of Freedom (DOF)
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Definition: Number of independent coordinates required to define the configuration of a mechanism.
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Kutzbach’s Criterion (Planar):
$$ DOF = 3(n - 1) - 2j - h $$
Where:
$n$ = total links (including frame),
$j$ = number of lower pairs (1 DOF joints like revolute/prismatic),
$h$ = number of higher pairs (2 DOF joints like cam-follower).
- Gruebler’s Criterion:
$$ DOF = 3(n - 1) - 2j $$
Assumes no redundant constraints and all joints are 1 DOF.
[!CAUTION]
Gruebler’s fails for mechanisms with redundant constraints (e.g., parallel linkages). Use Kutzbach for general cases.
Grashof’s Law & Four-Bar Classification
- Law: For a 4-bar linkage with link lengths $s$ (shortest), $l$ (longest), $p, q$ (intermediate):
$$ s + l \leq p + q $$
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Classification:
| Condition | Type | Crank Possibility | |-----------------------------|---------------------------|-----------------------------------------------| | $$\displaystyle s + l < p + q $$ | Grashof | At least one crank can rotate continuously. | | $$\displaystyle s + l = p + q $$ | Parallelogram/Delta | Special cases; change point. | | $$\displaystyle s + l > p + q $$ | Non-Grashof | No continuous crank rotation; double rocker. |
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Inversions: Fixing different links yields distinct mechanisms:
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Crank-rocker (fixed longest/shortest).
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Double crank (fixed intermediate).
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Double rocker (non-Grashof).
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Inversions of Mechanisms
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Definition: Different mechanisms obtained by fixing (grounding) different links in a kinematic chain.
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Four-Bar Inversions:
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Input crank fixed → Oscillating output.
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Coupler fixed → Drag-link (e.g., automobile wiper).
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Output rocker fixed → Crank-rocker input.
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Double Slider Crank Inversions:
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Scotch yoke (slider fixed → crank oscillates).
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Oldham’s coupling (one slider fixed → parallel misalignment compensation).
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Elliptical trammel (both sliders fixed → point on coupler traces ellipse).
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[!TIP]
Past Paper Focus: Whitworth quick return (crank and slotted lever) is an inversion of crank and slotted lever mechanism.
2. Kinematic & Dynamic Analysis
Velocity & Acceleration Analysis
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Instantaneous Center (IC) Method:
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Definition: Point in a body with zero instantaneous velocity.
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Kennedy’s Theorem: Three bodies in plane have 3 ICs collinear.
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Velocity at any point: $$\displaystyle v = \omega \times r_{IC} $$.
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Steps:
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Locate all fixed ICs (IC between link & frame).
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Use Kennedy’s theorem for moving ICs.
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Compute $\omega$ from known velocity: $$\displaystyle \omega = v/r $$.
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[!DIAGRAM: CANVAS]
Slider-crank with ICs: $$\displaystyle I_{12} $$ (crank-ground), $$\displaystyle I_{23} $$ (coupler-ground), $$\displaystyle I_{13} $$ (crank-coupler).
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Relative Motion Method:
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Velocity: $$\displaystyle \vec{v}_B = \vec{v}_A + \vec{\omega}_{AB} \times \vec{r}_{B/A} $$.
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Acceleration:
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$$ \vec{a}_B = \vec{a}_A + \vec{\alpha}_{AB} \times \vec{r}_{B/A} + \vec{\omega}_{AB} \times (\vec{\omega}_{AB} \times \vec{r}_{B/A}) $$
+ **Coriolis component** if $$\displaystyle \vec{v}_{B/A} $$ exists: $$\displaystyle 2\vec{\omega}_{AB} \times \vec{v}_{B/A} $$.
Coriolis Acceleration
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Expression: $$\displaystyle \vec{a}_c = 2\vec{\omega} \times \vec{v}_{rel} $$.
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Magnitude: $$\displaystyle a_c = 2\omega v_{rel} $$.
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Direction: Perpendicular to $$\displaystyle \vec{v}_{rel} $$, rotated by $$\displaystyle 90^\circ $$ in direction of $\vec{\omega}$.
[!TIP]
Past Paper Alert: Derivation of Coriolis component is frequent (Jun 2025, Jun 2022).
D’Alembert’s Principle
- Statement: Inertia forces and external forces on a body form a system in dynamic equilibrium.
$$ \sum (\vec{F} - m\vec{a}) = 0 \quad \text{and} \quad \sum (\vec{T} - I\vec{\alpha}) = 0 $$
- Significance: Converts dynamics problem into static equivalent; used for force analysis in mechanisms.
Force Analysis in Mechanisms
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Steps:
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Draw free-body diagrams of each link.
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Apply D’Alembert’s principle (add inertia forces $-m\vec{a}$, $-I\vec{\alpha}$).
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Resolve forces at joints (two-component unknowns).
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Use loop equations for torque/power balance.
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Friction: Include in joint reactions; e.g., friction force $$\displaystyle F_f = \mu N $$.
3. Mechanism Synthesis
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Number Synthesis: Determines possible kinematic chains for given DOF and joints (using graph theory).
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Motion Synthesis: Designs linkages for specified motion (position, velocity, acceleration).
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Analytical Method (Freudenstein’s Equation):
For four-bar with input $$\displaystyle \theta_2 $$, output $$\displaystyle \theta_4 $$:
$$ K_1 \cos \theta_4 - K_2 \cos \theta_2 + K_3 \cos(\theta_2 - \theta_4) = K_4 $$
Where $$\displaystyle K_1 = \frac{d^2 + c^2 - a^2 - b^2}{2ab} $$, etc. (standard form).
Satisfy at specified $$\displaystyle \theta_2, \theta_4 $$ to find link ratios.
- Graphical Method: Use relative pole technique for precision points.
[!TIP]
Past Paper: Freudenstein’s equation for position/velocity/acceleration synthesis (Jun 2025).
4. Specific Mechanisms
Four-Bar Linkage
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Type Determination: Apply Grashof’s criterion.
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Kinematic Analysis:
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Position: Loop-closure equations (complex numbers or trigonometry).
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Velocity/Acceleration: Use IC method or relative motion.
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Slider-Crank Mechanism
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Displacement: $$\displaystyle x = r\cos\theta + \sqrt{l^2 - r^2\sin^2\theta} $$ (for crank length $r$, connecting rod $l$).
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Velocity: $$\displaystyle v = -r\omega\sin\theta + \frac{r^2\omega\sin\theta\cos\theta}{\sqrt{l^2 - r^2\sin^2\theta}} $$.
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Acceleration: Differentiate velocity.
Quick Return Mechanisms
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Whitworth Mechanism:
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Time Ratio: $$\displaystyle Q = \frac{\text{Cut time}}{\text{Return time}} = \frac{360^\circ - 2\alpha}{360^\circ + 2\alpha} $$, where $$\displaystyle \alpha = \cos^{-1}\left(\frac{R}{d}\right) $$, $R$ = crank radius, $d$ = distance from crank center to slotted lever pivot.
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Design: Given $Q$, $R$, find $d$: $$\displaystyle d = R / \cos\alpha $$, $$\displaystyle \alpha = \frac{180^\circ(Q-1)}{2(Q+1)} $$.
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Crank and Slotted Lever: Similar time ratio formula.
Double Slider Crank
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Applications: Elliptical trammel, Oldham’s coupling.
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Inversions: See Section 1.
5. Cam Systems
Classification & Terminology
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Cams: Disk, plate, cylindrical, end face, conical.
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Followers:
| Type | Motion Axis | Pressure Angle | |-------------------|----------------------|-------------------| | Knife-edge | Through cam center | High wear | | Roller | Offset/through | Low wear | | Flat-faced | Through/offset | Low wear |
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Key Terms:
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Base circle: Smallest cam radius.
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Pitch circle: Circle through follower pitch point.
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Pressure angle $\phi$: Angle between follower motion and normal to cam profile.
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$$\tan\phi = \frac{\text{transverse component}}{\text{radial component}}$$
- Stroke: Maximum follower displacement $h$.
Follower Motions & Displacement Diagrams
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Uniform Velocity: $$\displaystyle s = \frac{h}{\beta}\theta $$ (linear diagram).
- $$\displaystyle v_{max} = \frac{h\omega}{\beta} $$, $$\displaystyle a = 0 $$ (except at transitions → infinite).
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Simple Harmonic Motion (SHM):
$$ s = \frac{h}{2}\left(1 - \cos\frac{\pi\theta}{\beta}\right) $$
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$$\displaystyle v = \frac{\pi h \omega}{2\beta}\sin\frac{\pi\theta}{\beta} $$,
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$$\displaystyle a = \frac{\pi^2 h \omega^2}{2\beta^2}\cos\frac{\pi\theta}{\beta} $$.
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$$\displaystyle v_{max} = \frac{\pi h \omega}{2\beta} $$, $$\displaystyle a_{max} = \frac{\pi^2 h \omega^2}{2\beta^2} $$.
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Uniform Acceleration/Deceleration:
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Rise/fall in $\beta/2$ each: $$\displaystyle s = \frac{2h}{\beta^2}\theta^2 $$ (first half), $$\displaystyle s = h - \frac{2h}{\beta^2}(\beta-\theta)^2 $$ (second half).
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$$\displaystyle v_{max} = \frac{2h\omega}{\beta} $$, $$\displaystyle a_{max} = \frac{4h\omega^2}{\beta^2} $$.
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Cam Profile Design
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Knife-edge: Inverse of displacement diagram (offset if follower axis offset).
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Roller: Add roller radius to base circle → pitch curve; offset by roller radius normal to pitch curve.
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Flat-faced: Tangential to pitch curve; ensure no undercut.
[!CAUTION]
Undercutting: Occurs if $$\displaystyle \phi > \phi_{max} $$ (typically $$\displaystyle 30^\circ $$ for slow, $$\displaystyle 15^\circ $$ for high speed). Reduces contact area.
Design Considerations
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Pressure Angle: Keep $$\displaystyle \phi < \phi_{allow} $$ to avoid high side thrust.
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Undercutting: Avoid by increasing base circle or modifying motion.
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Critical Path Motion: Path where follower velocity/acceleration peaks; design for minimum $\phi$.
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Torque on Cam Shaft: $$\displaystyle T = F_t \cdot r_{pitch} $$, where $$\displaystyle F_t $$ = tangential force.
6. Gear Systems
Fundamentals of Gearing
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Law of Gearing: Common normal to tooth profiles at point of contact passes through pitch point (instantaneous center).
Proof: For constant velocity ratio, $$\displaystyle \frac{\omega_1}{\omega_2} = \frac{r_2}{r_1} = \text{constant} $$.
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Conjugate Profiles: Profiles satisfying law of gearing (e.g., involute, cycloidal).
Involute Gear Geometry
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Parameters (for module $m$, pressure angle $\phi$):
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Addendum $$\displaystyle a = m $$, Dedendum $$\displaystyle d = 1.25m $$ (standard).
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Circular pitch $$\displaystyle p_c = \pi m $$.
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Base circle radius $$\displaystyle r_b = r \cos\phi $$.
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Path of Contact: Line along which contact occurs; length $$\displaystyle = \sqrt{r_{a1}^2 - r_{b1}^2} + \sqrt{r_{a2}^2 - r_{b2}^2} - (r_{b2} - r_{b1})\tan\phi $$.
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Arc of Contact: Path of contact / $\cos\phi$.
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Contact Ratio $\epsilon$:
$$ \epsilon = \frac{\text{Path of contact}}{p_c} $$
$$\displaystyle \epsilon > 1 $$ ensures smooth operation (typical $$\displaystyle \epsilon = 1.2–2 $$).
Interference & Undercutting
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Interference: Addendum tip of pinion contacts gear root before engagement ends.
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Avoidance: Minimum pinion teeth $$\displaystyle T_{min} = \frac{2r_a}{m}\sin^2\phi $$ (for full-depth teeth).
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For $$\displaystyle 20^\circ $$, $$\displaystyle T_{min} \approx 18 $$.
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Undercutting: Gear tooth trimmed near root to avoid interference; weakens tooth.
Gear Types
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Spur: Parallel axes, straight teeth.
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Helical: Helical teeth, gradual engagement ($$\displaystyle \phi_b = \tan^{-1}(\tan\phi/\cos\psi) $$).
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Bevel: Intersecting axes (conical).
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Worm: High reduction, non-intersecting perpendicular axes.
Gear Trains
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Simple: Each gear on separate shaft; $$\displaystyle \omega_{out}/\omega_{in} = \prod (N_{in}/N_{out}) $$.
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Compound: Multiple gears on same shaft; same as simple but intermediate shafts compound.
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Epicyclic (Sun-Planet):
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Velocity Ratio: Use Tabular Method or Aronson’s Method.
Tabular: Fix ring → count teeth for arm speed; then add arm speed.
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Torque: $$\displaystyle T_{sun} \cdot \omega_{sun} + T_{ring} \cdot \omega_{ring} + T_{arm} \cdot \omega_{arm} = 0 $$ (power balance).
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7. Power Transmission Elements
Belt Drives
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Open Belt: $$\displaystyle T_1/T_2 = e^{\mu\theta} $$ (where $\theta$ in radians, angle of lap on smaller pulley).
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Cross Belt: $$\displaystyle T_1/T_2 = e^{\mu\pi} $$ (if $$\displaystyle \theta = \pi $$).
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Belt Stress: $$\displaystyle \sigma = \frac{T}{b \cdot t} $$ (max tension $$\displaystyle T_1 $$).
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Power Transmitted: $$\displaystyle P = (T_1 - T_2)v $$.
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Maximum Power Condition: $$\displaystyle T_1 = T_{max} $$, $$\displaystyle T_2 = T_{max}/e^{\mu\theta} $$, $$\displaystyle v = \sqrt{\frac{T_{max}}{3\rho}} $$ (where $\rho$ = density).
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Slip & Creep:
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Slip: $$\displaystyle s = \frac{v_1 - v_2}{v_1} \times 100\% $$.
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Creep: Local deformation; $$\displaystyle s = \frac{\Delta l}{l} $$.
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Friction Devices
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Clutches:
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Plate Clutch (uniform pressure): $$\displaystyle T = \frac{2}{3}\mu W \frac{r_o^3 - r_i^3}{r_o^2 - r_i^2} $$.
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Plate Clutch (uniform wear): $$\displaystyle T = \mu W \frac{r_o^2 + r_i^2}{2(r_o - r_i)} $$.
[!BOX]
Uniform Wear Torque: $$\displaystyle T = \frac{\mu W}{2}(r_o + r_i) $$.
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Cone Clutch: $$\displaystyle T = \frac{\mu W \sin\alpha}{\sin\alpha + \mu\cos\alpha} \cdot \frac{r_o^2 + r_i^2}{2(r_o - r_i)} $$.
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Brakes:
- Band & Block:
$$ \frac{T_0}{T_n} = \left(\frac{1 + \mu\tan\theta}{1 - \mu\tan\theta}\right)^n $$
Where $n$ = number of blocks, $2\theta$ = angle subtended by each block.
> [!TIP]
> **Past Paper**: Derivation of band & block tension ratio (Jun 2025).
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Block Brake: $$\displaystyle T = \mu W R \frac{1 + \mu f}{1 - \mu f} $$ (with lever arm $f$).
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Disk Brake: $$\displaystyle T = 2\mu F R_{eff} $$ (two pads).
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Power Screws:
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Torque (raising): $$\displaystyle T = W \frac{d_m}{2} \tan(\phi + \lambda) $$, where $\lambda$ = lead angle, $\phi$ = friction angle.
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Efficiency: $$\displaystyle \eta = \frac{\tan\lambda}{\tan(\phi + \lambda)} $$ (square thread).
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Dynamometers:
- Prony Brake: $$\displaystyle P = W L \omega $$ (where $L$ = lever length, $W$ = force, $\omega$ = angular speed).
8. Vibrations & Balancing
Free Vibrations
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Longitudinal: Axial vibrations in rods/shafts; $$\displaystyle \omega_n = \sqrt{\frac{EA}{\rho A L^2}} = \sqrt{\frac{E}{\rho}} \cdot \frac{\pi}{L} $$.
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Transverse: Beam vibrations; $$\displaystyle \omega_n = \sqrt{\frac{EI}{\rho A L^4}} \cdot \beta^2 $$ (depends on end conditions).
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Torsional: Shaft twist; $$\displaystyle \omega_n = \sqrt{\frac{GJ}{\rho J_p L^2}} = \sqrt{\frac{G}{\rho}} \cdot \frac{\pi}{L} $$.
Balancing of Rotating Masses
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Static Balancing: Single plane; $$\displaystyle \sum m_i r_i = 0 $$ (vector sum).
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Dynamic Balancing: Two planes;
$$ \sum m_i r_i = 0, \quad \sum m_i r_i x_i = 0 $$
Where $$\displaystyle x_i $$ = axial distance from reference plane.
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Procedure for Multi-plane:
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Choose two balancing planes (X, Y).
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Write force and moment equations about X, Y.
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Solve for $$\displaystyle M_X, \theta_X $$ and $$\displaystyle M_Y, \theta_Y $$.
[!BOX]
Balance Mass: $$\displaystyle M = \sqrt{M_X^2 + M_Y^2} $$, $$\displaystyle \theta = \tan^{-1}(M_Y/M_X) $$.
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9. Dynamic Analysis Applications
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Force Analysis in Mechanisms: Combine inertia forces (from acceleration analysis) with external loads; use D’Alembert’s to find joint reactions and input torque.
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Torque in Clutches/Brakes: As above.
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Power in Power Screws/Belts: $$\displaystyle P = T\omega $$ or $$\displaystyle P = (T_1 - T_2)v $$.
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Critical Speed: For shafts, $$\displaystyle N_c = \frac{1}{2\pi}\sqrt{\frac{g}{\delta}} $$ (where $\delta$ = deflection).
Key Formulas Summary
| Topic | Formula |
|---|---|
| Kutzbach DOF | $3(n-1) - 2j - h$ |
| Grashof | $s + l \leq p + q$ |
| Whitworth Time Ratio | $$\displaystyle Q = \frac{360 - 2\alpha}{360 + 2\alpha} $$, $$\displaystyle \alpha = \cos^{-1}(R/d) $$ |
| SHM Displacement | $$\displaystyle s = \frac{h}{2}(1 - \cos\frac{\pi\theta}{\beta}) $$ |
| Belt Tension (open) | $$\displaystyle T_1/T_2 = e^{\mu\theta} $$ |
| Plate Clutch (wear) | $$\displaystyle T = \frac{\mu W}{2}(r_o + r_i) $$ |
| Band & Block | $$\displaystyle T_0/T_n = \left(\frac{1+\mu\tan\theta}{1-\mu\tan\theta}\right)^n $$ |
| Contact Ratio | $$\displaystyle \epsilon = \frac{\text{Path of contact}}{p_c} $$ |
| Power Screw Torque | $$\displaystyle T = W \frac{d_m}{2} \tan(\phi + \lambda) $$ |
Past Paper Hotspots
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Jun 2025: Whitworth design, Freudenstein synthesis, cam max velocity/acceleration, band brake derivation, plate clutch pressure, balancing mass.
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Dec 2024: Grashof type determination, epicyclic gear teeth numbers, belt stress (open/cross), Coriolis derivation.
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Jun 2024: Double slider crank inversions, tangent cam design, cam classification, belt power transmission.
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Jun 2023: Inversions, D’Alembert, cam displacement diagrams, gear contact ratio, Prony brake.
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Nov 2023: Constrained motion, Whitworth, slider-crank torque, cam profile SHM, belt selection, gear types.
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Jun 2022: Grashof, slip/creep, quick return distance, 4-bar type/velocity, epicyclic speed, cam acceleration, balancing.
[!FINAL TIP]
Exam Strategy: For numericals, always sketch the mechanism first. For derivations, state assumptions (e.g., uniform wear in clutches). For synthesis, clearly list given specs and unknowns.
These notes consolidate all high-frequency topics from RGPV past papers. Focus on derivations (Coriolis, band brake, law of gearing), numericals (belt stress, cam motions, balancing), and diagram-based questions (IC method, cam profiles, gear geometry).