Newton's Second Law for Rotation — Question 4

Section 10-8 · Physics pages 1518–1519

Question 4 A compound drum uses different moment arms for its cords A fixed compound drum has inertia 0.50 kg m2 and coaxial radii 0.30 and 0.20 m. Tangential cord forces of 12 and 8 N respectively produce positive and negative torques. 12 N 8 N Two upward tangential forces act on opposite sides and different radii. (a) Find its angular acceleration and each rim's signed tangential acceleration. (b) Can one subtract the cord forces before multiplying by a single radius?
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Question 4 - Solution A compound drum uses different moment arms for its cords 12 N 8 N (a) Derivation and calculation Each cord force must be multiplied by its own radius: τnet = 12(0.30) −8(0.20) = 2.0 N m. α = 2.0 0.50 = 4.0 rad/s2 , at,o = 0.30(4) = 1.20 , at,i = 0.20(4) = 0.80 m/s2 . These tangential components use the positive local angular tangent at each rim. (b) Result and interpretation The correct moment difference is FoRo −FiRi̸ = (Fo −Fi)R for an arbitrary common R. There is no shared application radius for the two forces, so subtracting forces first loses the lever-arm information. Physical check The larger radius has the larger tangential acceleration even though both rims share one angular acceleration.

Question 4

A compound drum uses different moment arms for its cords

A fixed compound drum has inertia 0.50kgm20.50\,\mathrm{kg\,m^2} and coaxial radii 0.300.30 and 0.20m0.20\,\mathrm m. Tangential cord forces of 1212 and 8N8\,\mathrm N respectively produce positive and negative torques.

Diagram shown in the original SVG worksheet.

  1. Find its angular acceleration and each rim's signed tangential acceleration.

  2. Can one subtract the cord forces before multiplying by a single radius?

Question 4 - Solution

A compound drum uses different moment arms for its cords

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Each cord force must be multiplied by its own radius: τnet=12(0.30)−8(0.20)=2.0Nm.\tau_{\mathrm{net}}=12(0.30)-8(0.20)=2.0\ \mathrm{N\,m}. α=2.00.50=4.0rad/s2,at,o=0.30(4)=1.20,at,i=0.20(4)=0.80m/s2.\boxed{\alpha=\frac{2.0}{0.50}=4.0\ \mathrm{rad/s^2}},\qquad \boxed{a_{t,o}=0.30(4)=1.20},\quad\boxed{a_{t,i}=0.20(4)=0.80\ \mathrm{m/s^2}}. These tangential components use the positive local angular tangent at each rim.

(b) Result and interpretation

The correct moment difference is FoRo−FiRi≠(Fo−Fi)Rfor an arbitrary common R.F_oR_o-F_iR_i\ne(F_o-F_i)R\quad\text{for an arbitrary common }R. There is no shared application radius for the two forces, so subtracting forces first loses the lever-arm information.

Physical check

The larger radius has the larger tangential acceleration even though both rims share one angular acceleration.