The center of mass of a semicircular arc of non-negligible width

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Homework Help Overview

The discussion revolves around finding the center of mass of a semicircular arc that has a non-negligible width. Participants are exploring the implications of the arc's geometry and mass distribution on the calculation of the center of mass.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss setting up a Riemann sum to approximate the center of mass, dividing the arc into sub-arcs and considering their individual contributions. There are questions about the accuracy of approximating the center of mass of each sub-arc and the implications of the arc's width on these calculations. Some suggest using polar coordinates for simplification, while others propose considering the semicircular slab approach as an alternative.

Discussion Status

The discussion is active, with various approaches being explored. Some participants have offered guidance on alternative methods and highlighted potential errors in reasoning regarding the center of mass calculations. There is recognition of the complexity introduced by the arc's width and the symmetry of the shape.

Contextual Notes

Participants are working under the constraints of a homework problem, which may limit the information available and the methods that can be employed. The discussion includes assumptions about the geometry and mass distribution of the semicircular arc.

Hamza M khan
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Homework Statement
The goal: finding the center of mas a semicircular wire/disk of on non negligible width, with the inner radius being R1 and out radius being R2.

My attempt:

1) Im gonna start this with a goal of setting up a reimann sum. First I divide the "arc"(?) of angle pi into n sub-arcs of equal angle Δθ

2) The total center of mass can be found if centers of mass of parts of the system are known. In each circular arc interval, I choose a height, Hi, approximating the height of the center os mass of each sub arc, hoping that the error goes to 0 in the limit as n goes to infinity, and multiply this by the mass of the sub arc. Pushing this through the limiting process, I set up the integral of H w.r.t m

3) finding Hi . Now, as Δθ goes to 0, the sector-difference region formed by each sub-arc should get closer and closer to a tilted rectangle. Assuming that to be true, the center of mass of each sub-arc( being approximated by a titled rectangle) would be a distance Hi=(R1+R2)sin(θ)/2 above the origin

4) lastly, since the shape has a constant mass per unit area, the differential mass and total mass can be replaced by differential area and total area. Using the sector area formula for each subinterval, the differntial area, dA, should be equal to 0.5dθ (R2^2-R1^2)

solving this gives me ycom=(R1+R2)/pi which upon looking up is clearly wrong. It is interesting thought that it gives the correct result when R1=R2 ( 0 thickness). What is the error in my reasoning?
Relevant Equations
Ycom=m1y1+m2y2+....miyi
My attempt:

1) I am going to start this with a goal of setting up a reimann sum. First I divide the "arc"(?) of angle pi into n sub-arcs of equal angle Δθ

2) The total center of mass can be found if centers of mass of parts of the system are known. In each circular arc interval, I choose a height, Hi, approximating the height of the center os mass of each sub arc, hoping that the error goes to 0 in the limit as n goes to infinity, and multiply this by the mass of the sub arc. Pushing this through the limiting process, I set up the integral of H w.r.t m

3) finding Hi . Now, as Δθ goes to 0, the sector-difference region formed by each sub-arc should get closer and closer to a tilted rectangle. Assuming that to be true, the center of mass of each sub-arc( being approximated by a titled rectangle) would be a distance Hi=(R1+R2)sin(θ)/2 above the origin

4) lastly, since the shape has a constant mass per unit area, the differential mass and total mass can be replaced by differential area and total area. Using the sector area formula for each subinterval, the differential area, dA, should be equal to 0.5dθ (R2^2-R1^2)

solving this gives me ycom=(R1+R2)/pi which upon looking up is clearly wrong. It is interesting thought that it gives the correct result when R1=R2 ( 0 thickness). What is the error in my reasoning?
 

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Hamza M khan said:
3) finding Hi . Now, as Δθ goes to 0, the sector-difference region formed by each sub-arc should get closer and closer to a tilted rectangle. Assuming that to be true, the center of mass of each sub-arc( being approximated by a titled rectangle) would be a distance Hi=(R1+R2)sin(θ)/2 above the origin
No matter how small you make ##\Delta \theta##, the center of mass of the sub-arc will not be at a radial distance of ##(R_1+R_2)/2##. The width of the sub-arc is greater at ##R_2## than at ##R_1##.

You could find the correct location of the CM of a sub-arc and then proceed as you did. However, it might be easier not to bother with the sub-arcs.
 
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Since the object has a constant thickness and a symmetrical shape, using a polar coordinate system would simplify calculations very much.

I agree with @TSny, your section has more area or mass above a line of arithmetic mean.
Basically, to exactly calculate the radius of the centroid for any infinitesimal section, you have two circular sectors to consider, the smaller one to be voided.

Since that section is symmetrical, the centroid will be located over the symmetry line of that section.
Please, see:
https://en.m.wikipedia.org/wiki/List_of_centroids

The location of the centroid of any shape of that kind must be dependent on the angle of the arc (which seems to be π in your schematic).
 
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A different approach would be to find the center of mass of a semicircular slab. That's straightforward to do even in cartesian coordinates. Then consider the arc as a slab of radius R2 minus the slab of radius R1.
 
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