Fluid Mechanics: Cone-Plate viscometer

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Homework Help Overview

The discussion revolves around the calculation of differential surface area for a cone in the context of fluid mechanics, specifically related to a cone-plate viscometer. Participants are exploring the relationships between various geometric elements and their implications for fluid dynamics.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the derivation of the differential surface area for a cone, questioning how to relate the radius of a strip element to the overall geometry of the cone. There are attempts to clarify the formula for the surface area of a truncated cone and its application to the problem at hand.

Discussion Status

There is an ongoing exploration of different methods to derive the differential area element, with some participants providing explanations and others questioning the necessity of certain steps. Multiple interpretations of the variables involved are being discussed, indicating a productive exchange of ideas.

Contextual Notes

Participants are navigating potential confusion regarding the definitions of variables and the geometric relationships within the cone. There is a mention of assumptions about the cone's dimensions and the nature of the differential elements being considered.

Feodalherren
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Homework Statement


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Homework Equations


Fluid Mechanics

τ =μ (du/dy)

The Attempt at a Solution



I got far enough to write down

dM = μ (Ωr/tanθ) dA

from just substitutions, easy enough.

I get confused when I'm solving for the differential surface area. I somehow need the dA for a cone.
For a circle it's easy enough. A=πr^2 so then dA = 2πr dr.

But how do I go about getting this for a cone? the book lists it as (2πr/cosθ) dr, without any explanation, of course.
 
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Take a strip element 2πxdr, where x is the radius of circle formed by that strip element. Try relating x to r using similarity of triangles.
 
Well you should first understand how to find the surface area of a "truncated cone" (ignoring the faces)
It is the average circumference of the cone multiplied by the side length (not the height)

So the surface area of a truncated cone (ignoring the faces) is 2\pi r_{avg}L or you could say 2\pi L\frac{r_1+r_2}{2}
(Side note, this also applies to normal cones; just treat the tip as r2=0)

So with this understanding of truncated cones, look at the following picture I made:
coneintegral.png

The differential surface area would be 2\pi r_{avg}L but as you can see from the picture, L=\frac{dr}{\cos\theta} therefore the differential surface area is \frac{2\pi R_{avg}}{\cos\theta}dr

The two radii are r and (r+dr) but since dr is obviously infinitesimal, it suffices to say r_{avg}=r
 
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Does it really require all that? Isn't using similarity to relate x and R, considering a string element of radius x, just enough?
 
erisedk said:
Does it really require all that? Isn't using similarity to relate x and R, considering a string element of radius x, just enough?
No that is incorrect. The differential area element is \frac{2\pi x}{\cos\theta}dx

Me and the OP were using r not to represent the radius of the base of the cone, but to represent what you called "x"
 
Nathanael said:
No that is incorrect. The differential area element is \frac{2\pi x}{\cos\theta}dx

Me and the OP were using r not to represent the radius of the base of the cone, but to represent what you called "x"

Oh ok.
 
Nathanael said:
Well you should first understand how to find the surface area of a "truncated cone" (ignoring the faces)
It is the average circumference of the cone multiplied by the side length (not the height)

So the surface area of a truncated cone (ignoring the faces) is 2\pi r_{avg}L or you could say 2\pi L\frac{r_1+r_2}{2}
(Side note, this also applies to normal cones; just treat the tip as r2=0)

So with this understanding of truncated cones, look at the following picture I made:
View attachment 78118
The differential surface area would be 2\pi r_{avg}L but as you can see from the picture, L=\frac{dr}{\cos\theta} therefore the differential surface area is \frac{2\pi R_{avg}}{\cos\theta}dr

The two radii are r and (r+dr) but since dr is obviously infinitesimal, it is suffices to say r_{avg}=r
Excellent explanation. Thank you very much, Sir.
 

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