Thermal physics problem on steel bar

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Homework Help Overview

The problem involves a thermal physics scenario with a steel bar and a copper bar connected end-to-end, where the temperature at one end of the steel bar is maintained at 100°C and the other end of the copper bar at 0°C. The objective is to find the temperature at the junction of the two bars and the total rate of heat flow.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the heat transfer equations and the relationship between the heat flow through the two bars. There is uncertainty about the correct application of the heat flow equations and the assumptions made regarding the lengths of the bars.

Discussion Status

Some participants have provided guidance on correcting the equations used to find the temperature at the junction. There is an ongoing exploration of how to calculate the total rate of heat flow, with some participants expressing uncertainty about the methods to use.

Contextual Notes

Participants note confusion regarding the application of heat flow principles, particularly in relation to the differing lengths of the bars and the implications for heat transfer calculations.

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[SOLVED] Thermal physics problem

Homework Statement



A steel bar 10cm long is welded end-to-end to a copper bar 20cm long. Both bars are insulated perfectly along their sides. Each bar has a radius of 2.0cm. The free end of the steel bar is maintained at 100^{o}C and the free end of the copper bar is maintained at 0^{o}C. Find the temperature at the junction between the two bars and the total rate of flow of heat.

k_{steel}=50.2Wm^{-1}K^{-1}
k_{copper}=385.0Wm^{-1}K^{-1}

Homework Equations



H = \frac{dQ}{dt} = -kA\frac{dT}{dx}

The Attempt at a Solution



Copper:

\frac{dQ}{dt} = \frac{-kA(373-T)}{L} = \frac{-385\pi(2X10^{-2})^{2}(273-T)}{20X10^{-2}}

Where T is the point at the junction between the bars, piXr^{2} has been substituted in for A, and 273K = 0C

so \frac{dQ}{dt} = -2.42(273-T)Steel:

\frac{dQ}{dt} = \frac{-50.2\pi(2X10^{-2})^{2}(373-T)}{10X10^{-2}}

As 373K = 100C

so \frac{dQ}{dt} = -0.63(373-T)

I then said H_{copper} = H_{steel} which I'm not sure is correct as in the example I was given in class the two bars were of equal length, but continued with the following:

2.42(273-T)=0.63(373-T)
2.42T-0.63T=660.4-235.3

T=\frac{425.1}{1.79}= 238K

I'm not sure this is right as it is less than the temperature of the free end of the copper bar and surely the result should be between 273K and 373K?
Also I don't know where to start on finding the total rate of flow of heat... The only thing I could think of was adding the individual heat flows together but I'm sure there's more to it than that.
 
Last edited:
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2.42(273-T)=0.63(373-T) This step is wrong. Rewright as 2.42(T- 273)=0.63(373-T) Now solve fro T.
 
Fantastic, thanks! 294K, that sounds better =)
How would I start going about finding the total rate of flow of heat?
I'm still not sure what to use for that.
 
Rate of flow of heat through the compound conductor is given by
delta(Q)/delta(t) = A*delta(T)/( l1/k1 + l2/k2)
 
Brilliant, thanks, I can't find that in my lecture notes -anywhere-.
I'll try it.
 
Ok I got 50.0W, that sounds sensible.
Thanks again!
 

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