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SCIENCE · INVESTIGATE AND EXPLAIN

Check units and boundaries before trusting a model

Build a thermal resistance ledger and separate power, flux and energy.

Learning outcome: Calculate a two-layer conduction prediction with consistent units and identify conditions that the model does not represent.

Starting recap

One watt is one joule per second. A temperature difference of one kelvin equals a difference of one Celsius degree.

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Try

The default panel transfers 75 W. Its area is 0.5 m² and the calculation assumes maintained surface temperatures.

Open the experiment

Predict

Predict total resistance, heat flux and energy transferred in ten minutes. Explain whether the layer powers should be added.

Experiment

Capture the default 30 mm and 0.1 W/(m K) case. Calculate both resistances, total rate and interface temperature on paper. Change second-layer thickness to 20 mm and then 40 mm with conductivity fixed; compare the whole-panel rates.

Conduct heat through two layers

Worked teaching model · synthetic values · Steady one-dimensional conduction through two uniform layers in series, area 0.5 m². Layer 1 is 20 mm thick with conductivity 0.2 W/(m K). Maintained outer surface temperatures are 80 and 20 °C; they are not ambient air temperatures. Perfect thermal contact, no lateral losses, internal heat generation, temperature dependence, convection or radiation. The temperature profile is already established; no warm-up time, heat capacity or real insulation rating is inferred. Layer 2 properties are synthetic teaching choices.

Reset keeps your prediction, captures and practice history.

Temperature (°C) · fixed outer surface temperatures020406080100010203040506070Layer 1Layer 2Position through the layers (mm), not time

At the interface the temperature is continuous because perfect contact is assumed. A change in slope reflects a change in conductivity; it does not represent energy accumulation.

Equal heat rates, separate temperature drops
LayerThickness (mm)Conductivity (W/(m K))Resistance (K/W)Left temperature (°C)Right temperature (°C)Drop (K)Heat rate (W)
Layer 1200.2000.20080.00065.00015.00075.000
Layer 2300.1000.60065.00020.00045.00075.000

Heat travels from the maintained 80 °C surface to the maintained 20 °C surface. Energy entering equals energy leaving: there is no net energy storage in either layer at steady state. The hot source supplies 75.000 W and the cold sink removes the same rate.

Steady heat-transfer rate 75.000 W; interface temperature 65.000 °C.

The same 75.000 J/s crosses each layer. Total resistance 0.800 K/W; heat flux 150.000 W/m². In ten minutes at these maintained conditions, 45.000 kJ passes through the assembly, not twice that amount.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Make a prediction that can survive a unit check

A panel result of “75” is incomplete. Is it watts, joules or watts per square metre? Those quantities answer different questions. Power P is energy transferred each second, measured in watts: 1 W = 1 J/s. Energy Q is the amount transferred over an interval, measured in joules. Heat flux is power per area, measured in W/m². Confusing them can make a design comparison appear successful while answering the wrong requirement.

Start with the default investigation: second-layer thickness 30 mm and conductivity 0.1 W/(m K). The area is 0.5 m². The fixed first layer is 20 mm thick with conductivity 0.2 W/(m K). Both outer surface temperatures are maintained, at 80°C and 20°C. Predict resistance, power and ten-minute energy before reading the ledger.

Convert lengths before building the model

Divide millimetres by 1,000 to obtain metres: 30 mm = 0.030 m and 20 mm = 0.020 m. The temperature difference is 60 K. A difference of 60 Celsius degrees also equals 60 K; this statement concerns a difference, not an absolute temperature conversion.

For each layer, R = L/(kA). Here R is thermal resistance in K/W, L is thickness in m, k is conductivity in W/(m K), and A is area in m². Check the units: metres divided by W m/K gives K/W. The first resistance is 0.020/(0.2 × 0.5) = 0.2 K/W. The second is 0.030/(0.1 × 0.5) = 0.6 K/W.

The total resistance is 0.8 K/W. Dividing the 60 K difference by this resistance gives P = 75 W. This is a rate through the whole panel. The interface temperature is 80 − 75 × 0.2 = 65°C; checking from the cold side gives 20 + 75 × 0.6 = 65°C. Agreement checks the shared boundary between the layers.

Keep the same transfer from being counted twice

At steady state, each successive layer transfers 75 W. Adding them to report 150 W would count the same energy twice. By contrast, dividing by area is appropriate when asking for flux: 75/0.5 = 150 W/m². The similar-looking number now has a different unit and meaning.

Ten minutes is 600 seconds. At the maintained rate, Q = P × time = 75 × 600 = 45,000 J, or 45 kJ. This is energy passing through the assembly. The model does not say the panel stores that amount, warms by a particular temperature or consumes a particular battery fraction. It contains no heat capacity or electrical source.

Test sensitivity without changing the question

Hold conductivity at 0.1 and compare second-layer thicknesses 20 mm and 40 mm. The second resistance doubles from 0.4 to 0.8 K/W, but total resistance changes from 0.6 to 1.0 K/W because the fixed layer remains. The rate changes from 100 W to 60 W, not to 50 W. Capture both profiles and explain the non-halving result with the unchanged first layer.

The OpenStax conduction mechanism supplies the slab relationship. Our two-layer arithmetic assumes steady one-dimensional conduction, uniform properties, perfect contact and no sideways loss. Outer face temperatures are not automatically room-air temperatures. Convection, radiation, contact resistance or a metal bypass would require additional relations. Changing a parameter inside a valid model differs from changing the situation so the model no longer applies.

Transfer: identify a missing boundary

A colleague keeps the default resistances but proposes maintained faces at 70°C and 20°C. On paper, predict the new power and energy transferred over 600 seconds. Then consider a different statement: “The room is 20°C and a container starts at 70°C.” Does that statement justify the same constant-rate energy calculation?

Check the changed-boundary transfer

With maintained faces, the difference is 50 K, giving 50/0.8 = 62.5 W and 37,500 J = 37.5 kJ over 600 seconds. A container starting at 70°C can cool; its face temperature is not maintained merely because the initial temperature was stated. Room temperature also need not equal the outside face temperature. A transient and surface-exchange model would be needed. These paper conditions extend the explanation; the widget does not change its fixed temperatures.

Write the assumptions beside your numerical answer. Return to temperature and heat if rate and stored energy remain confusing, then examine calibration and fair comparisons. A unit-correct answer is necessary, but it is only useful when its boundary conditions match the question.

Apply

A steady panel transfers 75 W for 600 seconds. How much energy passes through the whole assembly?

Public practice checks a specific claim. It does not establish independent mastery.

State which conditions permit multiplying power by 600 seconds. Explain why changing room temperature or adding a metal bypass requires a new boundary or geometry.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

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