Two identical aluminum plates with thickness of \(30 \mathrm{~cm}\) are pressed against each other at an average pressure of \(1 \mathrm{~atm}\). The interface, sandwiched between the two plates, is filled with glycerin. On the left outer surface, it is subjected to a uniform heat flux of \(7800 \mathrm{~W} / \mathrm{m}^{2}\) at a constant temperature of \(50^{\circ} \mathrm{C}\). On the right outer surface, the temperature is maintained constant at \(30^{\circ} \mathrm{C}\). Determine the thermal contact conductance of the glycerin at the interface, if the thermal conductivity of the aluminum plates is \(237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Discuss whether the value of the thermal contact conductance is reasonable or not.

Heat transfer is a fundamental concept in thermal sciences that involves the movement of thermal energy from one place to another due to temperature differences. It ensures that warmer areas transfer energy to cooler ones until thermal equilibrium is achieved. There are three primary modes of heat transfer: conduction, convection, and radiation.

In the context of the given exercise featuring aluminum plates and glycerin, conduction is the key mode of interest. Conduction occurs when the thermal energy is transferred through a material without the actual movement of the substance. This is what's happening when the heat is passed from the hotter side of an aluminum plate, through the glycerin, to the cooler side.

Understanding heat transfer is crucial when attempting to determine the efficiency and rate at which heat is conducted through different materials, as well as when selecting materials for engineering applications where temperature control is vital.

Fourier's Law of heat conduction is a principle that quantifies the heat flux passing through a material as a result of a temperature gradient. It is expressed mathematically by the equation:
\[q = -k \frac{\Delta T}{d}\]
where:

• \(q\) is the heat flux (the amount of heat transferred per unit area per unit time),
• \(k\) is the thermal conductivity of the material (a measure of its ability to conduct heat),
• \(\Delta T\) is the temperature difference across the material, and
• \(d\) is the thickness of the material.

Fourier's Law is the cornerstone of heat conduction analysis and provides a foundation for solving engineering problems involving thermal energy transfer. This relationship is applied in the textbook exercise to calculate the heat transfer through the aluminum plates.

Thermal conductivity, denoted as \(k\), is a material property that indicates how well a substance can conduct heat. It is defined as the amount of heat that passes through a unit area of the material with a unit temperature gradient per unit time. The SI unit for thermal conductivity is watts per meter per Kelvin (W/m·K).

Different materials have different thermal conductivities. For example, metals typically have high thermal conductivities, which means they are good conductors of heat, while materials like wood or plastic have low thermal conductivities, making them good insulators.

In our exercise, we are told that the thermal conductivity of the aluminum plates is \(237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), indicating aluminum's excellent ability to conduct heat, which is expected given its metallic nature.

Calculating the temperature difference is a straightforward yet essential process in thermal analysis. It is the driving force behind heat transfer by conduction and is represented by the symbol \(\Delta T\), indicating the difference between the temperatures of two points.

In the given exercise, the temperature difference calculation is the first step, being the difference between the uniform heat flux applied to one side of the aluminum plates and the maintained temperature on the other side. Precisely, the temperature difference across the glycerin layer is \(20^\circ \mathrm{C}\).

Knowing the temperature difference allows us to apply Fourier's Law of heat conduction effectively and to predict the behavior of heat flow through the materials involved, an important aspect when addressing real-world engineering challenges.