How Does Water Pressure Change Inside a Spinning Test Tube?

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SUMMARY

The pressure within a spinning test tube filled with water can be expressed as P = (1/2)ρω²(r² - r₀²), where ρ represents the water density, ω is the angular velocity, r is the radius at which pressure is being calculated, and r₀ is the radius of the free surface. The derivation involves recognizing that the acceleration due to circular motion is a = ω²r, leading to the differential pressure equation dP = -ρω²r dr. A common point of confusion arises when integrating pressure changes with respect to axis orientation, particularly when defining limits of integration.

PREREQUISITES
  • Understanding of circular motion dynamics
  • Familiarity with pressure differential equations
  • Knowledge of calculus, specifically integration techniques
  • Basic principles of fluid mechanics
NEXT STEPS
  • Study the derivation of pressure in rotating fluids using the Navier-Stokes equations
  • Explore the concept of angular momentum in fluid dynamics
  • Learn about the effects of axis orientation on integration limits in physics problems
  • Investigate the relationship between pressure and depth in static fluids
USEFUL FOR

Students and educators in physics, particularly those focusing on fluid dynamics and rotational motion, as well as anyone seeking to deepen their understanding of pressure changes in rotating systems.

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Homework Statement


A test tube filled with water is being spun around in an ultra centrifuge with angular velocity ω. The test tube is lying along a radius, and the free surface of the water is at a radius r0.

(a) Show that the pressure at radius r within the test tube is P = (1/2)rho*ω2(r2-r02). Ignore gravity and atmospheric pressure


Homework Equations


dP= -ρgdz


The Attempt at a Solution


Since the test tube is undergoing circular motion, and the water within the test the test tube lies at a varying radius from center, the acceleration (g) is given by a=(v2)/r = ω2r

So dP = -ρgdz = -ρω2rdr

P= -(1/2)ρω2r2 from r to r0

I think that much is fine, and this gives me the correct answer... But, here is where my understanding is hazy. If I define r to be increasing radially from center, then it is my understanding that my lower bound should be r and my upper to be r0.

Here's my question: If I define an axis to be increasing in one direction, then should I always integrate from the lower value to higher?

If I use this same reasoning with a simple pressure vs. water depth example then I run into trouble. If I want to find the pressure at a depth of 30m and I define my z axis to be increasing upwards then it seems to me the integral should look like this:

dP = ∫-ρgdz from -30 to 0 = -ρg(0 - -30) = -ρg*30

But the answer should be positive!

Any help would be much appreciated
 
Physics news on Phys.org
In the formula you have used, the gravitational acceleration is pointing in the negative z direction. If you change the direction of the axis, then you must also change the direction of the field.
 

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