Problem 21
Question
At temperature \(T_{0}\), two metal strips of length \(l_{0}\) and thickness \(d\), is bolted so that their ends coincide. The upper strip is made up of metal \(A\) and have coefficient of expansion \(\alpha_{A}\) and lower strip is made up of metal \(B\) with coefficient of expansion \(\alpha_{B} \cdot\left(\alpha_{A}>\alpha_{B}\right)\). When temperature of their blastic strip is in-seased from \(T_{0}\) to \(\left(T_{0}+\Delta T\right)\), on strip become longer than the other and blastic strip is bend in the form of a circle as shown in fig. Calculate the radius of furvature \(R\) of the strip: (a) \(R:=\frac{\left[2+\left(\alpha_{A}+\alpha_{B}\right) \Delta T\right] d}{2\left(\alpha_{A}-\alpha_{B}\right) \Delta T}\) (b) \(R=\frac{\left[2-\left(\alpha_{A}+\alpha_{B}\right) \Delta T\right] d}{2\left(\alpha_{A}-\alpha_{B}\right) \Delta T}\) (c) \(R=\frac{\left[2+\left(\alpha_{A}-\alpha_{B}\right) \Delta T\right] d}{2\left(\alpha_{A}-\alpha_{B}\right) \Delta T_{i}}\) (d) \(R=\frac{\left[2-\left(\alpha_{A}-\alpha_{B}\right) \Delta T\right] d}{2\left(\alpha_{A}-\alpha_{B}\right) \Delta \mathcal{k}}\)
Step-by-Step Solution
VerifiedKey Concepts
Thermal Expansion
For a solid, linear thermal expansion is often the primary concern, encompassing changes along one dimension as temperature shifts. This is calculated using the formula \( \Delta l = l_0 \alpha \Delta T \), where \( \Delta l \) is the change in length, \( l_0 \) is the original length, \( \alpha \) is the coefficient of linear expansion, and \( \Delta T \) is the change in temperature. This describes how a material's dimensions change due to thermal fluctuations, which can be crucial in engineering applications such as construction or machinery, where precise dimensions are necessary. Understanding thermal expansion is key in predicting how a material will behave under thermal stress.
Coefficient of Expansion
- **Linear Coefficient of Expansion (\( \alpha \))**: Describes changes in one-dimensional length.
- **Area Coefficient of Expansion**: Describes changes in two-dimensional area.
- **Volume Coefficient of Expansion**: Describes changes in three-dimensional volume.
For bimetallic strips, different metals have unique coefficients, causing one metal to expand more than the other when heated, leading to bending. This difference in expansion can be harnessed in devices like thermostats, where the bend of the strip opens or closes an electrical circuit.
Radius of Curvature
In our current exercise, the expression for the radius of curvature involves the thickness of the strip and the relative expansion difference between the two metals. Mathematically, it can be expressed as:\[ R = \frac{[2 + (\alpha_A + \alpha_B) \Delta T] d}{2 (\alpha_A - \alpha_B) \Delta T} \]Where \( R \) is the radius of curvature, \( d \) is the thickness, and \( \Delta T \) is the temperature change. Notice that this depends on the coefficients of expansion \( \alpha_A \) and \( \alpha_B \).
Understanding the radius of curvature in bimetallic strips is vital in precision instruments and applications where the bending needs to trigger specific mechanical or electrical responses. This principle is employed in diverse fields from engineering to modern smart technology devices.