Newton's Second Law for Rotation — Question 10

Section 10-8 · Physics pages 1530–1531

Question 10 Speed-dependent resistance produces an asymptotic terminal rate A rotor with I = 1.0 kg m2 starts at rest under constant drive torque 2.0 N m. Resistance is −bω with b = 0.50 N m s. t ω 4 Schematic approach to terminal angular speed; the equation sets the time scale. (a) Solve for angular velocity and find when it reaches half its terminal value. (b) Find initial acceleration and explain whether the terminal rate is reached at finite time.
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Question 10 - Solution Speed-dependent resistance produces an asymptotic terminal rate t ω 4 (a) Derivation and calculation The fixed-axis equation with linear resistance is I ˙ω = τ0 −bω, ˙ω + b I ω = τ0 I . Solving with ω(0) = 0 yields ω(t) = τ0 b (1 −e−bt/I) = 4(1 −e−t/2) rad/s . ω = 1 2ω∞⇒e−t/2 = 1 2 ⇒t1/2 = 2 ln 2 = 1.386 s . (b) Result and interpretation Differentiate the solution: α(t) = 2e−t/2 rad/s2, α(0) = 2.0 rad/s2 . For every finite t, e−t/2 > 0, so ω(t) < 4 rad/s. The terminal rate is the limiting balance τ0 −bω∞= 0 ⇒ω∞= 4 rad/s . Physical check The time constant I/b = 2 s has time units, and the initial rate of acceleration is τ0/I.

Question 10

Speed-dependent resistance produces an asymptotic terminal rate

A rotor with I=1.0kgm2I=1.0\,\mathrm{kg\,m^2} starts at rest under constant drive torque 2.0Nm2.0\,\mathrm{N\,m}. Resistance is −bω-b\omega with b=0.50Nmsb=0.50\,\mathrm{N\,m\,s}.

Diagram shown in the original SVG worksheet.

  1. Solve for angular velocity and find when it reaches half its terminal value.

  2. Find initial acceleration and explain whether the terminal rate is reached at finite time.

Question 10 - Solution

Speed-dependent resistance produces an asymptotic terminal rate

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The fixed-axis equation with linear resistance is Iω̇=τ0−bω,ω̇+bIω=τ0I.I\dot\omega=\tau_0-b\omega,\qquad \dot\omega+\frac bI\omega=\frac{\tau_0}I. Solving with ω(0)=0\omega(0)=0 yields ω(t)=τ0b(1−e−bt/I)=4(1−e−t/2)rad/s.\boxed{\omega(t)=\frac{\tau_0}{b}(1-e^{-bt/I}) =4(1-e^{-t/2})\ \mathrm{rad/s}}. ω=12ω∞⇒e−t/2=12⇒t1/2=2ln⁡2=1.386s.\omega=\tfrac12\omega_\infty\Rightarrow e^{-t/2}=\tfrac12 \Rightarrow\boxed{t_{1/2}=2\ln2=1.386\ \mathrm s}.

(b) Result and interpretation

Differentiate the solution: α(t)=2e−t/2rad/s2,α(0)=2.0rad/s2.\alpha(t)=2e^{-t/2}\ \mathrm{rad/s^2},\qquad\boxed{\alpha(0)=2.0\ \mathrm{rad/s^2}}. For every finite tt, e−t/2>0e^{-t/2}>0, so ω(t)<4\omega(t)<4 rad/s. The terminal rate is the limiting balance τ0−bω∞=0⇒ω∞=4rad/s.\tau_0-b\omega_\infty=0\Rightarrow\boxed{\omega_\infty=4\ \mathrm{rad/s}}.

Physical check

The time constant I/b=2I/b=2 s has time units, and the initial rate of acceleration is τ0/I\tau_0/I.