Question #56892

The outer edge of the grooved area of a long-playing record is at a radial distance 36 cm from the center; the inner edge is at a radial distance of 15 cm. The record rotates at 6.7 rev/min. The needle of the pick-up arm takes 2.3 minutes to move uniformly from the outer edge to the inner edge.
What is the radial speed of the needle?
m/s
What is the speed of the outer edge relative to the needle?
m/s
What is the speed of the inner edge relative to the needle?
m/s
Suppose the phonograph is turned off, and the record uniformly and stops rotating after 10 s. What is the angular acceleration?
rad/s2

Expert's answer

Answer on Question 56892, Physics, Mechanics, Relativity

Question:

The outer edge of the grooved area of a long-playing record is at a radial distance 36 cm36\,cm from the center; the inner edge is at a radial distance of 15 cm15\,cm. The record rotates at 6.7 rev/min6.7\,rev/min. The needle of the pick-up arm takes 2.3 minutes to move uniformly from the outer edge to the inner edge.

a) What is the radial speed of the needle?

b) What is the speed of the outer edge relative to the needle?

c) What is the speed of the inner edge relative to the needle?

d) Suppose the phonograph is turned off, and the record uniformly stops rotating after 10s10s. What is the angular acceleration?

Solution:

a) We can find the radial speed of the needle from the formula:


v=st,v = \frac{s}{t},


here, ss is the distance that the needle moves uniformly from the outer edge to the inner edge (in fact, it is the difference between outer and inner radial distances), tt is the time.

Substituting ss and tt into the previous formula we get:


v=st=(router−rinner)t=(0.36 m−0.15 m)2.3⋅60 s=0.21 m138 s=0.00152 ms=1.52⋅10−3 ms.v = \frac{s}{t} = \frac{(r_{outer} - r_{inner})}{t} = \frac{(0.36\,m - 0.15\,m)}{2.3 \cdot 60\,s} = \frac{0.21\,m}{138\,s} = 0.00152\, \frac{m}{s} = 1.52 \cdot 10^{-3}\, \frac{m}{s}.


b) Let's first convert rev/minrev/min to rad/srad/s:


ω=(6.7 revmin)⋅(2π rad1rev)⋅(1min60 s)=0.701 rads.\omega = \left(6.7\, \frac{rev}{min}\right) \cdot \left(2\pi\, \frac{rad}{1rev}\right) \cdot \left(\frac{1min}{60\,s}\right) = 0.701\, \frac{rad}{s}.


Then, from the relation between linear and angular variables we can find the speed of the outer edge relative to the needle:


vouter edge=router ω=0.36 m⋅0.701 rads=0.252 ms.v_{outer\,edge} = r_{outer}\, \omega = 0.36\,m \cdot 0.701\, \frac{rad}{s} = 0.252\, \frac{m}{s}.


c) Similarly, we can find the speed of the inner edge relative to the needle:


vinneredge=rinnerω=0.15m⋅0.701rads=0.105ms.v_{inner edge} = r_{inner} \omega = 0.15m \cdot 0.701 \frac{rad}{s} = 0.105 \frac{m}{s}.


d) By the definition, the angular acceleration is the change in the angular velocity, ω\omega, per unit of time, tt:


α=ΔωΔt=ωf−ωiΔt=0rads−0.701rads10s=−0.701rads10s=−0.0701rads2.\alpha = \frac{\Delta \omega}{\Delta t} = \frac{\omega_f - \omega_i}{\Delta t} = \frac{0 \frac{rad}{s} - 0.701 \frac{rad}{s}}{10s} = \frac{-0.701 \frac{rad}{s}}{10s} = -0.0701 \frac{rad}{s^2}.


The sign minus indicate that the record is slow down.

**Answer:**

a) v=1.52⋅10−3msv = 1.52 \cdot 10^{-3} \frac{m}{s}.

b) vouteredge=0.252msv_{outer edge} = 0.252 \frac{m}{s}.

c) vinneredge=0.105msv_{inner edge} = 0.105 \frac{m}{s}.

d) α=−0.0701rads2\alpha = -0.0701 \frac{rad}{s^2}.


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