A test-tube filled with a liquid and was swing around

In summary, a small cylindrical test-tube with inner radius R and initial liquid height h0 is connected by a long rope of length L (L»h0) and swinging horizontally with a constant angular velocity ω. The liquid is spraying out from a tiny round hole of radius r (r«R) at the bottom of the test-tube. The remaining height of the liquid as a function of time can be calculated using the continuity equation and circular motion equations. By equating the pressure at the bottom of the test-tube to the energy of the liquid exiting the hole, a first approximation for the velocity of the liquid can be found.
  • #1
rbwang1225
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0

Homework Statement


A small cylindrical test-tube of inner radius R is initially filled with a liquid up to height ##h_0##. The tube is connected by a long rope of length ##L## (##L»h_0##) and swinging horizontally with a constant angular velocity ##ω##. There is a tiny round hole of radius ##r## (##r « R##) at the bottom of the test-tube and the liquid is spraying out from the hole. What's the remaining height of the liquid as a function of time?
test-tube.png


Homework Equations


Continuity equation and circular motion equations.

The Attempt at a Solution


##v\pi r^2=wR\pi R^2##
##v=\frac{R^3ω}{r^2},##
where v is the speed of the liquid just outside the hole.
The small cube moving out the hole is ##dx\pi r^2## which is equal to the lose of the liquid in the tube ##dh \pi R^2.##
##v=\frac{dx}{dt}##
Then the remaining height of the liquid as a function of time is ##h(t)=h_0-∫dh=h_0-∫\frac{r^2}{R^2}dx=h_0-∫_0^t\frac{r^2}{R^2}\frac{R^3ω}{r^2}dt=h_0-Rωt##
I know I might miss something, could anyone point out for me.

Regards.
 
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  • #2
This is late and may be of no use, if so sorry.

Put a block of mass m in the bottom of a mass-less bucket. Attach a rope to the bucket as is done above with the test-tube and swing in a horizontal circle.

The force on the block is F = mv^2/r = mω^2r

The pressure of the block on the bottom of the bucket due to the block is,

F/Area of the block

With this you should be able to find the pressure at the bottom of the test tube? Now equate (the actual liquid velocity will be less but this is a good first approximation),

pressure*volume =

energy = ρ*volume*(velocity of liquid exiting hole)^2/2

Hope this helps (and is right!).
 

Related to A test-tube filled with a liquid and was swing around

1. What causes the liquid in the test tube to move when it is swung around?

The movement of the liquid in the test tube is due to centripetal force. This force is created when an object is moving in a circular motion and is directed towards the center of that motion.

2. Can the speed at which the test tube is swung affect the movement of the liquid?

Yes, the speed at which the test tube is swung can affect the movement of the liquid. The faster the test tube is swung, the greater the centripetal force and the more the liquid will move.

3. Does the type of liquid in the test tube affect its movement when swung around?

Yes, the type of liquid in the test tube can affect its movement. The density and viscosity of the liquid can impact the amount of force needed to move it and how quickly it will settle after being swung around.

4. What happens to the liquid when the test tube is swung upside down?

When the test tube is swung upside down, the liquid will move towards the top of the test tube. This is because of the centrifugal force created by the swinging motion, which pushes the liquid towards the outer edges of the tube.

5. Is there any practical use for swinging a test tube filled with liquid?

Yes, there are practical uses for swinging a test tube filled with liquid. This motion can be used to mix or separate substances, analyze the viscosity of a liquid, or demonstrate the principles of centripetal force in a physics experiment.

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