Centre of mass of a solid hemisphere.

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SUMMARY

The center of mass (CoM) of a uniform solid hemisphere with radius r is located at a distance of (3/8)r from the center of the flat face. The calculation involves using the integral formula for CoM, modified to account for the density and volume of thin discs stacked vertically. The volume element dV can be expressed as the area of the disc multiplied by its height, leading to the integral R = (1/M)∫ρy dV, where the integration is performed over the height of the discs.

PREREQUISITES
  • Understanding of integral calculus, specifically for calculating center of mass.
  • Familiarity with the concept of volume elements in three-dimensional geometry.
  • Knowledge of the properties of uniform solids and density.
  • Ability to visualize geometric shapes and their cross-sections.
NEXT STEPS
  • Study the derivation of the center of mass for different geometric shapes, such as spheres and cylinders.
  • Learn about the application of triple integrals in calculating volumes and centers of mass.
  • Explore the use of cylindrical coordinates in solving problems involving symmetry.
  • Practice problems involving the integration of functions to find areas and volumes of solids of revolution.
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grahammtb
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Hi there, I can't get my head round how to do the math for this problem. I'm sure it's not as hard as I think...

Homework Statement


Show that the CoM of a uniform solid hemisphere of radius r lies at a distance (3/8)r from the centre of the flat face.
You may find it convenient to regard the hemisphere as consisting of a very large number of extremely thin discs of varying radii stacked on top of each other.

Homework Equations


I'm thinking I'll need the equation for CoM, involving an integral: R=(1/M)\intrdm. This I think can be modified to: R=(1/M)\intr\rhodV, where rho is the density at radius r.

The Attempt at a Solution


N/A

Thanks very much for any help!
~Graham :wink:
 
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grahammtb said:
I'm thinking I'll need the equation for CoM, involving an integral: R=(1/M)\intrdm. This I think can be modified to: R=(1/M)\intr\rhodV, where rho is the density at radius r.
So far, so good. To avoid confusion, I recommend you use a different variable of integration than r--let's say y. (Imagine the hemisphere axis to be along the y-axis from y = 0 to y = r.) What's the volume of a thin disk located at position y?
 
Doc Al said:
So far, so good. To avoid confusion, I recommend you use a different variable of integration than r--let's say y. (Imagine the hemisphere axis to be along the y-axis from y = 0 to y = r.) What's the volume of a thin disk located at position y?

Ok, since the discs are extremely thin, I'd approximate the volume of the disc to be its area. So: A(y) = Pi.(r(y))2.
 
Hi Graham! :smile:
grahammtb said:
… You may find it convenient to regard the hemisphere as consisting of a very large number of extremely thin discs of varying radii stacked on top of each other.

… dV …

You're ignoring the hint …

if you use discs stacked on top of each other (with height z, say), you can go straight to integrating over dz, instead of dV. :wink:
 
grahammtb said:
Ok, since the discs are extremely thin, I'd approximate the volume of the disc to be its area. So: A(y) = Pi.(r(y))2.
The disks are thin, but not zero thickness! :bugeye: Hint: dV = Area dy.
 
Doc Al said:
The disks are thin, but not zero thickness! :bugeye: Hint: dV = Area dy.
Ah I think I see...so if dV = Ady, then I can put that into my original eqn. for CoM? R = (1/M)\int\rhoydV. Then R = (Pi.\rho/M)\inty3dy...I think :redface:
 
grahammtb said:
Ah I think I see...so if dV = Ady, then I can put that into my original eqn. for CoM? R = (1/M)\int\rhoydV. Then R = (Pi.\rho/M)\inty3dy...I think :redface:
You're on the right track, but not quite there yet. What's the radius of a disk at position y? (Draw yourself a diagram.)
 
yep! It worked! Thanks a lot guys, I'd have spent all afternoon trying to pick my way through :)
 

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