Question #84504

the tape in a video cassette has a total length 190 m and can play for 2.5 h. as the tape starts to play, the full reel has an outer radius of 36 mm and an inner radius of 14 mm. at some point during the play, both reels will have the same angular speed. what is the common angular speed? answer in units of rad/s
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Expert's answer

2019-01-28T15:46:07-0500

Answer on Question #84504 - Physics - Mechanics | Relativity

Problem

the tape in a video cassette has a total length 190m190\mathrm{m} and can play for 2.5h2.5\mathrm{h} . as the tape starts to play, the full reel has an outer radius of 36mm36\mathrm{mm} and an inner radius of 14mm14\mathrm{mm} . at some point during the play, both reels will have the same angular speed. what is the common angular speed? answer in units of rad/s

Solution.

l=190ml = 190m

t=2.5h=9000st = 2.5h = 9000s

R=36mm=0.36mR = 36mm = 0.36m

r=14mm=0.14mr = 14mm = 0.14m

w?w - ?


Fig 1

According to definition of angular velocity we will have:


w=vr,w = \frac {v}{r},


where vv - velocity of circling point, rr - radius of circle.

Velocity of circling point equally velocity of motion of the film, v=constv = \text{const} :


v=lt.v = \frac {l}{t}.


When r1=r2r_1 = r_2 , reels will have the same angular velocity (fig. 2)



Fig 2

We can use the law of mass conservation and find r1r_1 .

From Fig. 1:


M=Vρ=Shρ=(πR2πr2)hρ=πhρ(R2r2).M = \frac {V}{\rho} = \frac {S h}{\rho} = \frac {(\pi R ^ {2} - \pi r ^ {2}) h}{\rho} = \frac {\pi h}{\rho} (R ^ {2} - r ^ {2}).


From Fig. 2:


M=2m=2V1ρ=2S1hρ=2(πr12πr2)hρ=2πhρ(r12r2).M = 2 m = 2 \frac {V _ {1}}{\rho} = 2 \frac {S _ {1} h}{\rho} = 2 \frac {(\pi r _ {1} ^ {2} - \pi r ^ {2}) h}{\rho} = 2 \frac {\pi h}{\rho} (r _ {1} ^ {2} - r ^ {2}).


So,


πhρ(R2r2)=2πhρ(r12r2)\frac {\pi h}{\rho} (R ^ {2} - r ^ {2}) = 2 \frac {\pi h}{\rho} (r _ {1} ^ {2} - r ^ {2})R2r2=2(r12r2)R ^ {2} - r ^ {2} = 2 (r _ {1} ^ {2} - r ^ {2})R2r2=2r122r2R ^ {2} - r ^ {2} = 2 r _ {1} ^ {2} - 2 r ^ {2}2r12=R2r2+2r22 r _ {1} ^ {2} = R ^ {2} - r ^ {2} + 2 r ^ {2}2r12=R2+r22 r _ {1} ^ {2} = R ^ {2} + r ^ {2}r12=R2+r22r _ {1} ^ {2} = \frac {R ^ {2} + r ^ {2}}{2}r1=R2+r22.r _ {1} = \frac {\sqrt {R ^ {2} + r ^ {2}}}{\sqrt {2}}.


From (1):


w=vr1=ltr1=l2tR2+r2w = \frac {v}{r _ {1}} = \frac {l}{t r _ {1}} = \frac {l \sqrt {2}}{t \sqrt {R ^ {2} + r ^ {2}}}w=190290000.362+0.142=0.077 (rad/s)w = \frac {190 \sqrt {2}}{9000 \sqrt {0.36^{2} + 0.14^{2}}} = 0.077 \text{ (rad/s)}


Answer:


w=0.077 (rad/s)w = 0.077 \text{ (rad/s)}


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