Damped Simple Harmonic Motion — Question 9

Section 15-7 · Physics pages 2368–2369

Question 9 A contracting state path has an energy-based radius For a viscously damped oscillator with ω2 0 = k/m, define state coordinates X = x and Y = v/ω0. Let ρ2 = X2 + Y 2. X Y Scaled state trajectory winds clockwise inward; energy is proportional to the squared radius. (a) Derive d(ρ2)/dt and interpret it physically. (b) At a turning point and at an equilibrium crossing, compare the instantaneous contraction of ρ2. Does the state remain on an ellipse of fixed area?
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Question 9 - Solution A contracting state path has an energy-based radius X Y (a) Derivation and calculation ρ2 = x2 + v2/ω2 0, ˙v = −ω2 0x −2βv. dρ2 dt = 2xv + 2v ˙v ω2 0 = −4β v2 ω2 0 = −4βY 2 ≤0 . E = 1 2kρ2 ⇒˙E = −2kβv2/ω2 0 = −bv2. (b) Result and interpretation turning point: Y = 0 ⇒dρ2/dt = 0 ; equilibrium crossing: X = 0 ⇒dρ2/dt = −4βρ2 . The state follows an inward spiral rather than a fixed ellipse. Its radial contraction varies around a cycle even when the displacement envelope is exponential. Physical check When β = 0, the radius becomes constant and the conservative state circle is recovered.

Question 9

A contracting state path has an energy-based radius

For a viscously damped oscillator with ω02=k/m\omega_0^2=k/m, define state coordinates X=xX=x and Y=v/ω0Y=v/\omega_0. Let ρ2=X2+Y2\rho^2=X^2+Y^2.

Diagram shown in the original SVG worksheet.

  1. Derive d(ρ2)/dtd(\rho^2)/dt and interpret it physically.

  2. At a turning point and at an equilibrium crossing, compare the instantaneous contraction of ρ2\rho^2. Does the state remain on an ellipse of fixed area?

Question 9 - Solution

A contracting state path has an energy-based radius

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

ρ2=x2+v2/ω02,v̇=−ω02x−2βv.\rho^2=x^2+v^2/\omega_0^2,\qquad\dot v=-\omega_0^2x-2\beta v.dρ2dt=2xv+2vv̇ω02=−4βv2ω02=−4βY2≤0.\frac{d\rho^2}{dt}=2xv+\frac{2v\dot v}{\omega_0^2}=\boxed{-4\beta\frac{v^2}{\omega_0^2}=-4\beta Y^2\le0}.E=12kρ2⇒Ė=−2kβv2/ω02=−bv2.E=\tfrac12k\rho^2\Rightarrow\dot E=-2k\beta v^2/\omega_0^2=-bv^2.

(b) Result and interpretation

turning point: Y=0⇒dρ2/dt=0;\text{turning point: }Y=0\Rightarrow\boxed{d\rho^2/dt=0};equilibrium crossing: X=0⇒dρ2/dt=−4βρ2.\text{equilibrium crossing: }X=0\Rightarrow\boxed{d\rho^2/dt=-4\beta\rho^2}.The state follows an inward spiral rather than a fixed ellipse. Its radial contraction varies around a cycle even when the displacement envelope is exponential.

Physical check

When β=0\beta=0, the radius becomes constant and the conservative state circle is recovered.