1) Hickory dickory dock, the 20.0-g mouse ran up the clock, and took turns riding on the 0.20-m-long second hand, the 0.20-m-long minute hand and the 0.10-m-long hour hand. What was the angular momentum of the mouse on each of the three hands?

2) In a physics experiment, Ingrid, the ice skater, spins around in the rink at 1.2 m/s with each of her arms stretched out 0.70m from the center of her body. In each hand she holds a 1.0kg mass. If angular momentum is conserved, how fast will Ingrid beging to spin if she pulls her amrs to a position 0.15m from the center of her body?

Respuesta :

1a) Angular momentum of the mouse on the second hand: [tex]8.4\cdot 10^{-5} kg m^2/s[/tex]

The angular momentum of the mouse is given by:

[tex]L=mvr[/tex]

where

m = 20.0 g = 0.02 kg is the mass of the mouse

v is the speed of the mouse

r = 0.20 m is the length of the hand

The speed of the mouse is equal to the length of the circumference divided by the time taken to complete one circle (60 s):

[tex]v=\frac{2\pi r}{t}=\frac{2\pi (0.20 m)}{60 s}=0.021 m/s[/tex]

So the angular momentum is

[tex]L=mvr=(0.02 kg)(0.021 m/s)(0.2 m)=8.4\cdot 10^{-5} kg m^2/s[/tex]


1b) Angular momentum of the mouse on the minute hand: [tex]1.4\cdot 10^{-6} kg m^2/s[/tex]

In this case, the mouse takes [tex]60\cdot 60=3600 s[/tex] to complete one circle, so the speed of the mouse is

[tex]v=\frac{2\pi r}{t}=\frac{2 \pi (0.20 m)}{3600 s}=3.5\cdot 10^{-4} m/s[/tex]

So, the angular momentum is

[tex]L=mvr=(0.02 kg)(3.5\cdot 10^{-4} m/s)(0.20 m)=1.4\cdot 10^{-6} kg m^2/s[/tex]


1c) Angular momentum of the mouse on the hour hand: [tex]3\cdot 10^{-8} kg m^2/s[/tex]

In this case, the mouse takes [tex]60\cdot 60 \cdot 12=43200 s[/tex] to complete one circle, so the speed of the mouse is

[tex]v=\frac{2\pi r}{t}=\frac{2 \pi (0.10 m)}{43200 s}=1.5\cdot 10^{-5} m/s[/tex]

So, the angular momentum is

[tex]L=mvr=(0.02 kg)(1.5\cdot 10^{-5} m/s)(0.10 m)=3\cdot 10^{-8} kg m^2/s[/tex]


2) New speed of Ingrid: 5.6 m/s

The initial angular momentum of Ingrid is twice the momentum produced by each mass:

[tex]L_i=2 mvr = 2(1.0 kg)(1.2 m/s)(0.70 m)=1.68 kg m/s[/tex]

Angular momentum must be conserved, so the final momentum must be the same when the arms are pulled to a new length of r'=0.15 m, so we find:

[tex]L_f = L_i = 2 mv r'\\v=\frac{L_f}{2mr'}=\frac{1.68 kg m/s}{2(1.0 kg)(0.15 m)}=5.6 m/s[/tex]