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Show that the SI units of thermal conduc...

Show that the SI units of thermal conductivity are `W//m-K`.

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To show that the SI units of thermal conductivity (k) are \( \text{W/m·K} \), we will start with Fourier's law of heat conduction. ### Step-by-Step Solution: 1. **Understand Fourier's Law**: According to Fourier's law, the rate of heat transfer (Q) through a material is proportional to the negative temperature gradient. The formula is given by: \[ Q = -k \cdot A \cdot \frac{dT}{dx} \] where: - \( Q \) is the heat transfer rate (in Watts, W), - \( k \) is the thermal conductivity (in unknown units), - \( A \) is the cross-sectional area through which heat is being transferred (in square meters, m²), - \( \frac{dT}{dx} \) is the temperature gradient (in Kelvin per meter, K/m). 2. **Rearranging the Formula**: From the equation, we can express thermal conductivity (k) as: \[ k = \frac{Q}{A \cdot \frac{dT}{dx}} \] 3. **Identify the Units**: - The unit of heat transfer rate \( Q \) is Watts (W). - The unit of area \( A \) is square meters (m²). - The unit of temperature gradient \( \frac{dT}{dx} \) is Kelvin per meter (K/m). 4. **Substituting the Units**: Now, substituting these units into the equation for k: \[ k = \frac{\text{W}}{\text{m}^2 \cdot \left(\frac{\text{K}}{\text{m}}\right)} \] 5. **Simplifying the Units**: When we simplify the expression: \[ k = \frac{\text{W}}{\text{m}^2} \cdot \frac{\text{m}}{\text{K}} = \frac{\text{W}}{\text{m} \cdot \text{K}} \] 6. **Final Result**: Thus, we find that the SI unit of thermal conductivity \( k \) is: \[ k = \frac{\text{W}}{\text{m} \cdot \text{K}} \] ### Conclusion: The SI units of thermal conductivity are \( \text{W/m·K} \).

To show that the SI units of thermal conductivity (k) are \( \text{W/m·K} \), we will start with Fourier's law of heat conduction. ### Step-by-Step Solution: 1. **Understand Fourier's Law**: According to Fourier's law, the rate of heat transfer (Q) through a material is proportional to the negative temperature gradient. The formula is given by: \[ Q = -k \cdot A \cdot \frac{dT}{dx} ...
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