Lee's Disc experiment for Thermal Conductivities

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Discussion Overview

The discussion revolves around Lee's disc experiment for measuring thermal conductivities, specifically focusing on the methodology of removing the upper brass base during the experiment and its implications on the initial conditions and heat transfer dynamics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the rationale behind removing the upper brass base after reaching steady state, suggesting that it alters initial conditions by exposing the glass to air, which is a poor conductor.
  • Another participant argues that without the lower brass disk, the temperature distribution over the lower surface would be non-uniform due to convective heat transfer to the air, which is mitigated by the high thermal conductivity of brass.
  • A different perspective emphasizes that the goal is to measure the rate of heat loss from the lower brass plate, which is achieved by heating it and allowing it to cool without interference from the upper heated plate.
  • There is a clarification regarding the confusion over which brass piece is being removed, with one participant confirming they meant the upper piece, not the lower one.
  • Concerns are raised about whether adding an insulator on top effectively stops heat loss, given that glass conducts better than air, leading to a discussion on the relative importance of convection versus conduction in heat loss.
  • Another participant supports the idea that keeping the insulating disc will reduce convective heat loss from the top surface of the lower plate, although they acknowledge that some heat loss will still occur.
  • One participant suggests that the experiment could benefit from using a better insulator in the second half of the experiment.

Areas of Agreement / Disagreement

Participants express differing views on the effects of removing the upper brass base and the role of the insulating disc, indicating that multiple competing perspectives remain without a clear consensus.

Contextual Notes

Participants highlight the dependence on the thermal properties of materials involved, such as the differences in heat transfer mechanisms (conduction vs. convection) and the impact of initial conditions on the experiment's outcomes.

Who May Find This Useful

Readers interested in experimental physics, thermal conductivity measurements, and heat transfer principles may find this discussion relevant.

dreamLord
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Here is the experiment in brief for those uninitiated :
http://media.uws.ac.uk/~davison/labpage/leedisk/leedisk.html

My question is, when the steady state has been obtained (heat flowing into Brass Disc = heat flowing out of it), why do we remove the upper Brass Base and then heat the disc? Why not with it? We need to find the value of rate of fall of temperature at the steady state temperature T1 ; if we remove the Brass Base, are we not changing our initial conditions, since now the glass will be in direct contact with air, an extremely poor conductor, while in the other case it would have been in contact with Brass.

Is it because while obtaining the steady state, heat is flowing out of Base only in the downward direction, and we want the same to happen for the cooling curve? If so, why?

Thanks!
 
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dreamLord said:
if we remove the Brass Base, are we not changing our initial conditions, since now the glass will be in direct contact with air, an extremely poor conductor, while in the other case it would have been in contact with Brass.

Without the lower brass disk, the temperature over the lower surface of the disk would not be uniform, because of the convective heat transfer to the air. The temperature is made uniform by the high thermal conductivity of the brass.

Also, think about why the thermometers are "inside" the brass disks, and how you would measure the temperatures accurately without the disks. (Measuring the air temperature close to the bottom surface of the disk with a thermometer is no good).
 
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What you're trying to find is the rate of heat loss from the sides and bottom of the lower brass plate (since this is equal to the rate of heat entry, through the insulating disc, from the heated top brass plate). This rate of loss of heat is found by heating the bottom plate and letting it cool without heat being lost or gained through the upper surface. Hence no top heated plate, but retain the insulating disc to inhibit heat loss from the top surface of the lower brass plate.
 
AlephZero said:
Without the lower brass disk, the temperature over the lower surface of the disk would not be uniform, because of the convective heat transfer to the air. The temperature is made uniform by the high thermal conductivity of the brass.

I think my naming of the apparatus might have caused some confusion (I used the link). I am talking about removing the upper brass piece, not the lower one. Or maybe I don't follow what you are saying - can you dumb it down please?

Philip Wood said:
What you're trying to find is the rate of heat loss from the sides and bottom of the lower brass plate (since this is equal to the rate of heat entry, through the insulating disc, from the heated top brass plate). This rate of loss of heat is found by heating the bottom plate and letting it cool without heat being lost or gained through the upper surface. Hence no top heated plate, but retain the insulating disc to inhibit heat loss from the top surface of the lower brass plate.

I understand that we need to find the rate of heat loss from the sides and bottom of the lower brass piece. But does adding an insulator on the top really stop heat loss from the top? Glass is a better conductor than air, so if heat can flow down into the air(a worse conductor than glass), it should be able to flow up into the glass as well, right?
 
Right. But leaving on the insulating disc will help. Without the disc, the top surface of the bottom plate will lose heat mainly by convection - far more important than conduction here, because air is a very poor conductor. Of course, with the disc in place, there will still be some convective loss, as the top of the disc will be warm, but being a poor conductor the disc will have a large temperature difference between its two flat faces, i.e. the top face will be cooler than the top face of the bottom plate, so the convective heat loss rate will be reduced. Having said that, I've always thought that the experiment would benefit by use (in the second half) of a better insulator than the insulator being investigated in the first half!
 
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Ah, I think I understand. Thanks Philip and Alpeh!
 

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