A 2-cm-diameter plastic rod has a thermocouple inserted to measure temperature at the center of the rod. The plastic \(\operatorname{rod}\left(\rho=1190 \mathrm{~kg} / \mathrm{m}^{3}, c_{p}=1465 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right.\), and \(k=0.19 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) ) was initially heated to a uniform temperature of \(70^{\circ} \mathrm{C}\), and allowed to be cooled in ambient air temperature of \(25^{\circ} \mathrm{C}\). After \(1388 \mathrm{~s}\) of cooling, the thermocouple measured the temperature at the center of the rod to be \(30^{\circ} \mathrm{C}\). Determine the convection heat transfer coefficient for this process. Solve this problem using analytical one-term approximation method (not the Heisler charts).

In heat transfer analysis, the Fourier number (\textbf{Fo}) plays a critical role. It's a dimensionless number that indicates the ratio of heat conduction rate to the rate of thermal energy storage. If you're studying problems where heat conduction is transient, like heating up or cooling down of objects, the Fourier number will be your guide. It helps to understand how quickly a material responds to temperature changes. For the cylindrical plastic rod in our example, it's essentially a measure of how much time it takes for the rod to cool down relative to its thermal inertia.

For calculation purposes, Fourier number is given by the formula:
\[Fo = \frac{\alpha \cdot t}{L^2}\]
where \(\alpha\) is the thermal diffusivity, \(t\) is the time, and \(L\) is the characteristic length (the radius in the case of cylindrical objects). For our plastic rod example, with a calculated Fourier number of 0.124, we can infer that the rod cools down at a rate that makes our problem suitable for the one-term approximation method to provide a reasonable estimate of the temperature variation over time.

Similarly to the Fourier number, the Biot number (\textbf{Bi}) is another dimensionless number crucial in heat transfer problems, especially for transient conduction analysis. The Biot number compares the conductive heat transfer resistance within a body to the convective heat transfer resistance across the body's surface. This number shows whether an object can be assumed to have a uniform temperature throughout (if Bi is small) or if there are significant temperature gradients within it (if Bi is large).

The formula for Biot number is as follows:
\[Bi = \frac{h \cdot L}{k}\]
where \(h\) is the convection heat transfer coefficient, \(L\) is the characteristic length, and \(k\) is the thermal conductivity. Using our example problem, we deduced a Biot number of approximately 0.34, indicating that the temperature variation within the rod could reasonably be analyzed using the lumped capacitance method, where the temperature is assumed to be uniform across its cross-section at any given time.

Thermal diffusivity (\textbf{\(\alpha\)}) is the property of a material that characterizes the speed at which heat diffuses through it. It's a measure that brings together the material's density (\(\rho\)), specific heat capacity (\(c_p\)), and thermal conductivity (\(k\)) in one term that describes how quickly a material reacts to changes in temperature.

You can calculate thermal diffusivity using the equation:
\[\alpha = \frac{k}{\rho \cdot c_p}\]
For the 2-cm-diameter plastic rod we've been discussing, we determined the thermal diffusivity to be \(8.975 \times 10^{-8} m^2/s\). This value helped us in calculating the Fourier number and ultimately in analyzing the cooling process of the rod in conjunction with the Biot number.

The one-term approximation method is a mathematical simplification used in heat transfer to estimate temperature variations over time for bodies experiencing transient conduction. Generally, the precise temperature distribution within a body would require solving complex equations. For certain conditions, mainly when the product of the Biot number and the Fourier number is relatively small, the approximation that the temperature varies linearly with time becomes valid.

The general approach for using the one-term approximation method is to solve the equation:
\[\frac{T - T_\infty}{T_i - T_\infty} = \sum_{n=1}^{1} \frac{4}{(2n - 1)\pi} e^{-(2n - 1)^2\pi^2Bi\:Fo}\]
This assumes that the first term of the series provides a sufficiently accurate solution, and higher-order terms can be neglected. By applying this method to our plastic rod problem, we determined the Biot number and subsequently used it to calculate the convection heat transfer coefficient necessary for cooling the rod.