Hoop stress in solid disc from thermal contraction

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Discussion Overview

The discussion revolves around the hoop stresses in a solid disc resulting from thermal contraction, specifically focusing on a composite disc made of copper and silica. Participants explore the implications of thermal contraction on the disc's shape and stress distribution, referencing relevant equations and theories.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant seeks to understand how to convert thermal contraction into pressure for the thick-walled hoop equation, noting that the disc is solid with a radius of 40mm.
  • Another participant asks for clarification on whether the disc is a composite structure with copper bonded to silica, suggesting that the differing contraction rates could lead to a cup shape upon cooling.
  • A participant confirms that the copper is adhered to the silica and describes the resulting deformation when cooled, indicating a lift of around 1 mm at the edges.
  • A link to a relevant paper is provided, suggesting it may contain useful information regarding the topic.
  • Participants express appreciation for the resources shared and the responses received.

Areas of Agreement / Disagreement

Participants generally agree on the nature of the composite disc and the effects of thermal contraction, but the specifics of the stress calculations and implications remain unresolved.

Contextual Notes

There are limitations regarding the assumptions made about the material properties and the exact nature of the thermal contraction effects, which have not been fully explored or quantified in the discussion.

Who May Find This Useful

This discussion may be useful for individuals interested in materials science, mechanical engineering, or those studying the effects of thermal stresses in composite materials.

elrohir00
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Hi,

I have been looking at hoop stresses and the information I have found hasn't been all that useful to me as I am having a hard time converting the thermal contraction of a system into a pressure for the equation (stress=a+b/r^2). This is the thick walled hoop equation

The disc is a few microns of copper on 0.7mm silica and from the thermal contraction the disc bends from Stoney's equation. The discs are solid (no hole) and have a radius of 40mm.

as the disc is solid b=0 so we only have a which is apparently the pressure. As all of the stresses are coming from thermal contraction I'm not sure if it will all cancel out.

the radius of the copper contracts by 0.1304mm and the silica contract by 0.0032mm if its required.

Thanks for your time
 
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hello, elrohir.

Are you describing a composite disc where a complete layer of copper is bonded to a complete layer of silica, like a part sandwich?

So that if the composite disk is flat and cools the copper will contract more than the silica, pulling the disc into a cup shape?

Or have I misunderstood?
 
yes the copper is stuck onto the silica. At room temperature the disc is flat to a few nanometres and when its cooled it makes a cup/bowl shape and the edges lift by around 1 mm
 
http://www.iasmirt.org/SMiRT16/B1834.PDF

I think its also in Timoshenko "Theory of Plates and Shells"
 
Last edited by a moderator:
Thats looking right on the money. I will give it a read through and see what i can extract

Thanks studiot for a quick response
 
go well
 

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