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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 rA=250r_A = 250 mm and rB=100r_B = 100 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 −ma⃗ˉ-m\bar{\vec a} acting at the mass centre GG.
  • Inertia couple −Iˉα⃗-\bar I\vec\alpha (for plane motion).

For a rigid body in plane motion the equations of dynamic equilibrium are

∑Fx−maˉx=0,∑Fy−maˉy=0,∑MG−Iˉα=0\sum F_x - m\bar a_x = 0, \qquad \sum F_y - m\bar a_y = 0, \qquad \sum M_G - \bar I\alpha = 0

which are the same as ∑F⃗=ma⃗ˉ\sum \vec F = m\bar{\vec a} and ∑MG=Iˉα\sum M_G = \bar I\alpha, 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 (α=0\alpha=0): only the inertia force; rotation about a fixed axis through GG: only the inertia couple −Iα-I\alpha.

   real forces + (-m a) at G + (-I alpha) couple  =>  equilibrium

Numerical part

Data: mA=10m_A = 10 kg, kˉA=0.080\bar k_A = 0.080 m, rA=0.250r_A = 0.250 m, rB=0.100r_B = 0.100 m, M=8M = 8 N m on gear BB. The data give no mass for gear BB, so its inertia is neglected (if it is included, add IBI_B in the equations below). The tangential force between the teeth is FF.

IˉA=mAkˉA2=10(0.080)2=0.064 kg m2\bar I_A = m_A\bar k_A^2 = 10(0.080)^2 = 0.064\ \text{kg m}^2
        M (on B)
         ( B  )---F--->(tooth)
                      ( A )

(b) Tangential force on A

Gear BB (massless): M−FrB=0M - F r_B = 0

F=MrB=80.100=80.00 NF = \frac{M}{r_B} = \frac{8}{0.100} = 80.00\ \text{N}

(a) Time to reach 600 rpm

Gear AA: FrA=IˉAαAF r_A = \bar I_A\alpha_A

αA=FrAIˉA=80.00×0.2500.064=312.50 rad/s2\alpha_A = \frac{F r_A}{\bar I_A} = \frac{80.00\times0.250}{0.064} = 312.50\ \text{rad/s}^2

The teeth have the same tangential acceleration: αBrB=αArA\alpha_B r_B = \alpha_A r_A

αB=αArArB=312.50×0.2500.100=781.25 rad/s2\alpha_B = \alpha_A\frac{r_A}{r_B} = 312.50\times\frac{0.250}{0.100} = 781.25\ \text{rad/s}^2 ωB=600 rpm=600×2π60=62.83 rad/s,t=ωBαB=62.83781.25=0.0804 s\omega_B = 600\ \text{rpm} = \frac{600\times2\pi}{60} = 62.83\ \text{rad/s}, \qquad t = \frac{\omega_B}{\alpha_B} = \frac{62.83}{781.25} = 0.0804\ \text{s}

Answer: t=0.0804t = 0.0804 s; tangential force F=80.00F = 80.00 N.

✓ Answer checked by Claude Opus 5.5 (high effort)

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