- 2079 Baishakh · 4+8 marks
D'Alembert's principle; gears with couple
Short answer
D’Alembert’s principle adds reversed inertia force –m a at G and inertia couple –¯ I α to real forces, giving dynamic equilibrium: ∑F – m a = 0, ∑M_G – ¯ I α = 0. For the gears, the tangential force that gear B exerts on A is F = 80.00 N; the time for gear B to reach 600 rpm is t = 0.0804 s.
Explain D' Alemberts principle with necessary equations. Gear A has a mass of 10 kg and a radius of gyration of 80 mm. The system is at rest when a couple M of magnitude 8 Nm is applied to gear B. Neglecting friction. Take mm and mm. Determine: a) The time required for the angular velocity of gear C [sic, gear B] to reach 600 rpm. b) The tangential force which gear B exerts on gear A. [Figure: large gear A (radius 250 mm) meshing with small gear B (radius 100 mm); couple M on B.]
D'Alembert's principle converts a dynamics problem into a statics problem. A body in motion is in dynamic equilibrium if, in addition to the real forces and moments, we add inertia effects equal and opposite to the effective forces:
- Inertia force acting at the mass centre .
- Inertia couple (for plane motion).
For a rigid body in plane motion the equations of dynamic equilibrium are
which are the same as and , but written as "sum of forces including inertia terms is zero". The moment equation can then be taken about any point, as in statics. Special cases: pure translation (): only the inertia force; rotation about a fixed axis through : only the inertia couple .
real forces + (-m a) at G + (-I alpha) couple => equilibrium
Numerical part
Data: kg, m, m, m, N m on gear . The data give no mass for gear , so its inertia is neglected (if it is included, add in the equations below). The tangential force between the teeth is .
M (on B)
( B )---F--->(tooth)
( A )
(b) Tangential force on A
Gear (massless):
(a) Time to reach 600 rpm
Gear :
The teeth have the same tangential acceleration:
Answer: s; tangential force N.
✓ Answer checked by Claude Opus 5.5 (high effort)
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