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Vibrations and Waves - Tutorial Questions VnW1 · Vibrations and Waves (Nov-Dec 2017) Tutorial...

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Vibrations and Waves (Nov-Dec 2017) Tutorial Questions VnW1 (20/11-24/11/2017) Vibrations and Waves – Tutorial Questions VnW1 NOTE: This question is suggested as a possibility for tutorial work. Please do not attempt it until your tutor tells you to. QUESTION The heart of a mechanical watch is the balance — an oscillating wheel of radius R and mass m mounted on a very low friction bearing. A spiral spring (the hairspring) provides a restoring torque τ = -k θ where θ is the angular displacement of the balance wheel from its equilibrium position (θ = 0) and k is a spring constant. This mechanism is known as a “torsional oscillator”. Balance wheel and hairspring assembly from my wristwatch. (i) What are the units of k here? (ii) The moment of inertia of the balance wheel is I . Derive the equation of motion for the balance wheel. (iii) Show that θ(t )= A cos(ω 0 t +φ) and ˜ θ(t )= A exp[ i(ω 0 t +φ)] are both general solutions to the equation of motion, where A , ω 0 and φ are constants. Hence obtain an expression for the natural frequency of the system ω 0 and its period T . (iv) The moment of inertia of the wheel for rotation about its centre is I = mR 2 . The mass of the particular balance wheel shown above is m = 40 mg and its radius is R = 4.5 mm. Determine the spring constant k required to give the required period of 1/3 s. (v) Find the numerical values of A and φ that adapt the general solution θ(t )= A cos(ω 0 t + φ) to the following sets of initial conditions. Assume a value of ω 0 corresponding to a period of 1/3 s. (a) Balance wheel is rotated to θ = 4.5 rad (258 ) and then released at time t =0 with zero angular velocity. (b) Balance wheel at equilibrium position is given kick that gives it an initial angular velocity of 35.0 rad/s. (c) Sketch θ(t ) versus time, t for the solutions a) and b), clearly showing the ampli- tude and period of the motion. (vi) For the mass on spring system, we derived in the lectures the following expressions for the potential and kinetic energy PE = 1 2 k [x (t )] 2 , KE = 1 2 m[v (t )] 2 , where x (t ) and v (t )=dx / dt are the displacement and velocity of the mass, respectively. 1 of 2
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Page 1: Vibrations and Waves - Tutorial Questions VnW1 · Vibrations and Waves (Nov-Dec 2017) Tutorial Questions VnW1 (20/11-24/11/2017) Vibrations and Waves – Tutorial Questions VnW1 NOTE:

Vibrations and Waves (Nov-Dec 2017) Tutorial Questions VnW1 (20/11-24/11/2017)

Vibrations and Waves – Tutorial Questions VnW1NOTE: This question is suggested as a possibility for tutorial work. Please do notattempt it until your tutor tells you to.

QUESTION

The heart of a mechanical watch is the balance — an oscillating wheel of radius R andmass m mounted on a very low friction bearing. A spiral spring (the hairspring) provides arestoring torque τ = −kθ where θ is the angular displacement of the balance wheel fromits equilibrium position (θ = 0) and k is a spring constant. This mechanism is known as a“torsional oscillator”.

Balance wheel and hairspring assembly from my wristwatch.

(i) What are the units of k here?

(ii) The moment of inertia of the balance wheel is I. Derive the equation of motion for thebalance wheel.

(iii) Show that θ(t) = A cos(ω0t+φ) and θ̃(t) = A exp[ i(ω0t+φ)] are both general solutions tothe equation of motion, where A , ω0 and φ are constants. Hence obtain an expressionfor the natural frequency of the system ω0 and its period T .

(iv) The moment of inertia of the wheel for rotation about its centre is I = mR2. Themass of the particular balance wheel shown above is m = 40 mg and its radius isR = 4.5 mm. Determine the spring constant k required to give the required period of1/3 s.

(v) Find the numerical values of A and φ that adapt the general solution θ(t) = A cos(ω0t +φ) to the following sets of initial conditions. Assume a value of ω0 corresponding to aperiod of 1/3 s.

(a) Balance wheel is rotated to θ = 4.5 rad (≈ 258◦) and then released at time t = 0with zero angular velocity.

(b) Balance wheel at equilibrium position is given kick that gives it an initial angularvelocity of 35.0 rad/s.

(c) Sketch θ(t) versus time, t for the solutions a) and b), clearly showing the ampli-tude and period of the motion.

(vi) For the mass on spring system, we derived in the lectures the following expressionsfor the potential and kinetic energy PE = 1

2k [x(t)]2, KE = 12m[v(t)]2, where x(t) and

v(t) = dx/ dt are the displacement and velocity of the mass, respectively.

1 of 2

Page 2: Vibrations and Waves - Tutorial Questions VnW1 · Vibrations and Waves (Nov-Dec 2017) Tutorial Questions VnW1 (20/11-24/11/2017) Vibrations and Waves – Tutorial Questions VnW1 NOTE:

Vibrations and Waves (Nov-Dec 2017) Tutorial Questions VnW1 (20/11-24/11/2017)

(a) Using the normal connection between rotational and linear motion (i.e. x ↔ θand m ↔ I), derive a general expression for the total energy of the torsionaloscillator in terms of k , θ and I.

(b) Show that the equation of motion derived in (ii) can also be obtained from thefact that the total energy is conserved, i.e. it is constant with respect to time.

Paul Tangney 2 of 2


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