Which wall thickness gives half the stress

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Homework Help Overview

The discussion revolves around determining the wall thickness of a hollow tube that results in half the stress under a constant tension. The subject area includes concepts from mechanics and material science, particularly focusing on stress, strain, and the properties of materials as described by Young's Modulus.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between stress, area, and tension, questioning whether the extension in length or change in strain is necessary for solving the problem. There is discussion about the annular cross-sectional area of the tube and how it relates to the wall thickness and diameter.

Discussion Status

Participants are actively engaging with the problem, clarifying concepts related to stress and area. Some guidance has been offered regarding the annular cross-sectional area, and there is a recognition of the relationship between stress and area as participants work through their reasoning.

Contextual Notes

There is an emphasis on the constant circumference of the tube and the implications of changing wall thickness on the cross-sectional area. Participants are navigating through assumptions about the geometry of the tube and its impact on stress calculations.

Janiceleong26
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Homework Statement


image.jpg


Homework Equations


Young's Modulus, E=σ/ξ
Stress,σ =F/A
Strain, ξ=x/L

The Attempt at a Solution


As diameter and tension are constant, so stress must be constant I assume.. So for the same Young's modulus, if stress is halved, then strain must be halved too I guess. But I don't know what is the extension and length. Do we have to consider the increase in circumference?
 
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What does your second equation in your list of relevant equations tell you? Do you really need to know the extension in length to answer this question? Do you really need to know the change in strain to answer this question? They already said in the problem statement that the circumference πD stays constant, right?

Chet
 
Chestermiller said:
What does your second equation in your list of relevant equations tell you? Do you really need to know the extension in length to answer this question? Do you really need to know the change in strain to answer this question? They already said in the problem statement that the circumference πD stays constant, right?

Chet
F is directly proportional to A? Oh so if stress is halved, and for the same tension, area is halved right? But area of..? Is it the area of the thickness of the tube?
 
Janiceleong26 said:
F is directly proportional to A? Oh so if stress is halved, and for the same tension, area is halved right?
No. Try again, getting the math correct this time.

But area of..? Is it the area of the thickness of the tube?
The annular cross sectional area of the tube.
 
Chestermiller said:
No. Try again, getting the math correct this time.The annular cross sectional area of the tube.
Oh sorry, I mean area would double, not halved.
But I thought the diameter is the same?
 
Janiceleong26 said:
Oh sorry, I mean area would double, not halved.
But I thought the diameter is the same?
The diameter is the same, but the pipe is hollow and the wall thickness doubles. The cross sectional area is ##A = \pi D W##
 
Oh I see it now.. The annular cross sectional area of the tube is actually the area of a rectangle, if we cut the tube and straighten it out, right? Ok thanks !
 
Janiceleong26 said:
Oh I see it now.. The annular cross sectional area of the tube is actually the area of a rectangle, if we cut the tube and straighten it out, right? Ok thanks !
That's one way of looking at it. Another way is:

$$A=\frac{\pi D_{outer}^2}{4}-\frac{\pi D_{inner}^2}{4}=\pi \left(\frac{D_{outer}+D_{inner}}{2}\right)\left(\frac{D_{outer}-D_{inner}}{2}\right)=\pi D_{average}W$$
 
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Chestermiller said:
That's one way of looking at it. Another way is:

$$A=\frac{\pi D_{outer}^2}{4}-\frac{\pi D_{inner}^2}{4}=\pi \left(\frac{D_{outer}+D_{inner}}{2}\right)\left(\frac{D_{outer}-D_{inner}}{2}\right)=\pi D_{average}W$$
Ohh thanks!
 

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