Problem 267
Question
Suppose a solid object in \(\mathbb{R}^{3}\) has a temperature distribution given by \(T(x, y, z)\). The heat flow vector field in the object is \(\mathbf{F}=-k \nabla T,\) where \(k>0\) is a property of the material. The heat flow vector points in the direction opposite to that of the gradient, which is the direction of greatest temperature decrease. The divergence of the heat flow vector is \(\nabla \cdot \mathbf{F}=-k \nabla \cdot \nabla T=-k \nabla^{2} T\). Compute the divergence.
Step-by-Step Solution
Verified Answer
The divergence is \(-k \nabla^2 T\).
1Step 1: Understand the Given Information
We are given a solid object in \(\mathbb{R}^3\) with a temperature distribution \(T(x, y, z)\). The heat flow vector field is defined as \(\mathbf{F} = -k abla T\). We need to find the divergence of this vector field.
2Step 2: Set Up the Divergence Expression
The divergence of a vector field \(\mathbf{F}\) is given by \(abla \cdot \mathbf{F}\). Here, \(\mathbf{F} = -k abla T\), so the divergence becomes \(abla \cdot (-k abla T)\).
3Step 3: Apply Scalar and Vector Calculus Identity
The expression simplifies using linearity of the divergence operator: \(abla \cdot (c\mathbf{A}) = c(abla \cdot \mathbf{A})\) for any constant \(c\) and vector field \(\mathbf{A}\). Thus, \(-k abla \cdot abla T = -k abla^2 T\).
4Step 4: Interpret the Result
\(-k abla^2 T\) represents the divergence of the heat flow vector field \(\mathbf{F}\). Here, \(abla^2 T\) is the Laplacian of \(T\), representing diffusion-related terms in heat flow.
Key Concepts
DivergenceGradientLaplacian
Divergence
In vector calculus, divergence is a fundamental concept that describes how much a vector field spreads out from a particular point. Imagine you're tracing water flowing through a sponge. Divergence measures how much water is entering or leaving a given point in space. When calculating the divergence of a vector field \( \mathbf{F} \), you involve the dot product of the del operator (\( abla \)) and the vector field itself.
For instance, consider the exercise at hand where the heat flow vector field is \( \mathbf{F} = -k abla T \). The divergence of \( \mathbf{F} \) will tell us how the heat is spreading throughout the object. Using the linearity of divergence, where \( abla \cdot (c\mathbf{A}) = c(abla \cdot \mathbf{A}) \) for any constant \( c \) and vector \( \mathbf{A} \), the calculation simplifies to show how the temperature gradient affects the flow of heat.
For instance, consider the exercise at hand where the heat flow vector field is \( \mathbf{F} = -k abla T \). The divergence of \( \mathbf{F} \) will tell us how the heat is spreading throughout the object. Using the linearity of divergence, where \( abla \cdot (c\mathbf{A}) = c(abla \cdot \mathbf{A}) \) for any constant \( c \) and vector \( \mathbf{A} \), the calculation simplifies to show how the temperature gradient affects the flow of heat.
- A positive divergence indicates heat is spreading outwards from a point, warming the area.
- A negative divergence suggests heat is being 'sucked' inwards, cooling the region.
Gradient
The gradient is a critical tool in vector calculus to determine the rate and direction of change in a scalar field. Think of it as an arrow pointing in the direction of the steepest ascent on a hill; the length of the arrow indicates how fast you're climbing. In the context of our exercise, \( abla T \) represents the gradient of the temperature field \( T(x, y, z) \). This gradient vector points in the direction where the temperature increases most rapidly. For the given heat flow equation \( \mathbf{F} = -k abla T \), the negative sign indicates that the heat flow is in the direction opposite to the temperature increase, hence moving towards cooler areas.
- The magnitude of \( abla T \) reflects the intensity of the temperature change at any given point.
- The direction helps in visualizing how heat "desires" to distribute within the object.
Laplacian
The Laplacian is an operator that appears frequently in differential equations and modeling physical phenomena like heat conduction. It essentially extends the concept of the second derivative to functions of more than one variable, giving insight into how the function curves at a particular point.For the exercise, the Laplacian \( abla^2 T \) plays a pivotal role in understanding how heat diffuses across the object. The Laplacian of a scalar function, like temperature \( T \), is the divergence of the gradient (\( abla \cdot abla T \)). In simpler terms, it provides a measure of how a scalar field deviates from being flat or uniform.
- The Laplacian can be visualized as indicating whether a region is a peak or a trough in terms of heat distribution.
- A positive value suggests a local minimum, implying potential heat accumulation.
- A negative value often signals a local maximum, indicating heat is likely to be migrating away.
Other exercises in this chapter
Problem 264
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