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When you finish this section, you should be able to:
Recall that the partial derivatives of a function \(z=f(x,y)\) at the point \((x_{0},y_{0})\) are defined as \[ \begin{eqnarray*} f_{x}(x_{0},y_{0})&=&\lim_{\Delta x\rightarrow 0}\frac{f(x_{0}+\Delta x,y_{0})-f(x_{0},y_{0})}{\Delta x}\\ f_{y}(x_{0},y_{0})&=&\lim_{\Delta y\rightarrow 0}\frac{f(x_{0},y_{0}+\Delta y)-f(x_{0},y_{0})}{\Delta y} \end{eqnarray*} \]
where \((x_{0},y_{0})\) is an interior point of the domain of \(f\). The partial derivative \(f_{x}(x_{0},y_{0})\) equals the rate of change of \(f\) at \((x_{0},y_{0})\) in the direction of the positive \(x\)-axis, and the partial derivative \(f_{y}(x_{0},y_{0})\) equals the rate of change of \(f\) at \((x_{0},y_{0})\) in the direction of the positive \(y\)- axis. The directional derivative of \(f\) equals the rate of change of \(f\) at \((x_{0},y_{0})\) in any direction in the \(xy \)-plane.
To lay the groundwork for defining the directional derivative, we consider a function \(z=f( x,y)\) whose graph is a surface in space. In Figure 1, \(P_{0}=(x_{0},y_{0})\) is an interior point in the domain of \(f\), and \(\mathbf{u}=\cos \theta \mathbf{i}+\sin \theta \mathbf{j}\) is a unit vector in the \(xy\)-plane with its initial point at \(P_{0}\) making an angle \(\theta\), \(0\leq \theta \leq 2\pi\), with the positive \(x\)-axis.
Unit vectors are discussed in Section 10.3, pp. 708-709.
The vector \(\mathbf{u}\) allows us to move away from \(P_{0}\) in any direction. Now draw a directed line segment \(L\) with initial point \(P_{0}\) in the direction of \(\mathbf{u}\), and choose a point \(P=(x,y)\) on \(L\) different from \(P_{0}\), so that the directed line segment \(\overrightarrow{ P_{0}P}\) is in the domain of \(f\). Then \(\overrightarrow{P_{0}P}=t\mathbf{u}\) for some \(t\) and the coordinates of \(P\) are \((x_{0}+t\cos \theta ,y_{0}+t\sin \theta )\).
In Figure 2, we have drawn a surface \(z=f( x,y)\) and have labeled the points on the surface corresponding to \(P_{0}=( x_{0},y_{0}, 0)\), namely \(Q_{0}=( x_{0},y_{0},f( x_{0},y_{0}) )\), and to \(P=( x_{0}+t\cos \theta, y_{0}+t\sin \theta, 0)\), namely \(Q=(x_{0}+t\cos \theta, y_{0}+t\sin \theta\), \(f ( x_{0}+t\cos \theta ,y_{0}+t\sin \theta))\). The average rate of change of \(z\) with respect to \(t\) in the direction of \(\mathbf{u}=\cos \theta \mathbf{i} +\sin \theta \mathbf{j}\) is \[ \dfrac{\Delta z}{\Delta t}=\frac{f(x_{0}+t\cos \theta ,y_{0}+t\sin \theta)-f(x_{0},y_{0})}{t} \]
By taking the limit as \(t\rightarrow 0\), we obtain the rate of change of \(f\) at \((x_{0},y_{0})\) in the direction of \(\mathbf{u}\), provided the limit exists. This limit, denoted by \(D_{\mathbf{u}}f(x_{0},y_{0})\), is the directional derivative of \(f\) at \((x_{0},y_{0})\) in the direction of \(\mathbf{u}\).
Suppose \(z=f(x,y)\) is a function of two variables whose domain is \(D\) and \((x_{0},y_{0})\) is an interior point of \(D\). If \(\mathbf{u}=\cos \theta \mathbf{i}+\sin \theta \mathbf{j}\), \(0\leq \theta \leq 2\pi\), is a unit vector, the directional derivative of \(f\) at \((x_{0},y_{0})\) in the direction of \(\mathbf{u}\) is the number \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{D_{\mathbf{u}}f(x_{0},y_{0})=\lim\limits_{t \rightarrow 0}\dfrac{f(x_{0}+t\cos \theta ,y_{0}+t\sin \theta )-f(x_{0},y_{0})}{t}}} \]
provided the limit exists.
There are an infinite number of directions from \(P_{0}\) and so there are an infinite number of directional derivatives of \(f\) at the point \(( x_{0},y_{0})\). The directional derivative \(D_{\mathbf{u}}f( x_{0},y_{0})\) depends not only on the point \(( x_{0},y_{0})\), but also on the angle \(\theta\), the direction taken from \(( x_{0},y_{0})\). The partial derivatives \(f_{x}\) and \(f_{y}\) of \(f\) at \((x_{0},y_{0})\) are special cases of the directional derivative \(D_{\mathbf{u}}f(x_{0},y_{0})\), where the direction taken is \({\bf i}\) for \(f_{x}(x_{0},y_{0})\) and the direction taken is \({\bf j}\) for \(f_{y}(x_{0},y_{0})\). For example, if \(\theta =0\), then \[ \begin{equation*} \mathbf{u}=\cos 0\; \mathbf{i}+\sin 0\;\mathbf{j}=\mathbf{i} \end{equation*} \]
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Then using the definition of the directional derivative of \(f\) at \((x_{0},y_{0})\) in the direction \(\mathbf{u} =\mathbf{i}\), we find \[ \begin{equation*} D_{\mathbf{u}}f(x_{0},y_{0})=D_{{\bf i}}f(x_{0},y_{0})\underset{\color{#0066A7}{\theta =0}}{\underset{\color{#0066A7}{\uparrow} }{=}}\lim_{t\rightarrow 0}\frac{ f(x_{0}+t,y_{0})-f(x_{0},y_{0})}{t}=f_{x}(x_{0},y_{0}) \end{equation*} \]
Similarly, if \(\theta =\dfrac{\pi }{2}\), then \[ \begin{equation*} \mathbf{u=}\cos \dfrac{\pi }{2}\mathbf{i}+\sin \dfrac{\pi }{2}\mathbf{j}= \mathbf{j} \end{equation*} \]
and \[ \begin{equation*} D_{{\bf j}}f(x_{0},y_{0})=f_{y}(x_{0},y_{0}) \end{equation*} \]
Conditions under which a function \(z=f(x,y)\) is differentiable are discussed in Section 12.4, pp. 841-843.
Finding directional derivatives using the definition can be challenging. However, for functions \(z=f(x,y)\) that are differentiable, we can use the formula below to find directional derivatives.
If \(z=f(x,y)\) is a differentiable function, then the directional derivative of \(f\) at \((x_{0},y_{0})\) in the direction of the unit vector \(\mathbf{u}=\cos \theta \mathbf{i}+\sin \theta \mathbf{j}\) is given by \[ \begin{equation} \bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ D_{\mathbf{u}}f(x_{0},y_{0})=f_{x}(x_{0},y_{0})\cos \theta +f_{y}(x_{0},y_{0})\sin \theta }} \end{equation} \]
If \(x=x_0\,+\,t\cos \theta\), \(y=y_0\,+\,t\sin \theta\), and \(\theta\) is fixed, we can express \(z=f( x,y)\) as a function \(z= f(x_{0}+t \cos \theta, y_{0} + t \sin\theta)=g(t)\). Then the derivative of \(g\) at \(t=0\) is \[ \begin{eqnarray} g′ (0) &=& \lim\limits_{t\rightarrow 0}\dfrac{g(t)-g(0) }{t-0}=\lim_{t\rightarrow 0}\frac{f(x_{0}+t\cos \theta ,y_{0}+t\sin \theta )-f(x_{0},y_{0})}{t}\nonumber \\ &=& D_{\mathbf{u}}f(x_{0},y_{0}) \end{eqnarray} \]
Because \(f\) is differentiable, we can use Chain Rule I to find \(g′(t)\). \[ \begin{eqnarray*} g′ (t) &=&\frac{\partial f}{\partial x}\frac{dx}{dt}+\frac{\partial f}{ \partial y}\frac{dy}{dt} \qquad \color{#0066A7}{\hbox{Chain Rule I.}} \\ &=&\frac{\partial f}{\partial x}\cos \theta +\frac{\partial f}{\partial y} \sin \theta \quad\! \color{#0066A7}{\dfrac{dx}{dt}=\dfrac{d}{dt} (x_{0}+t\cos \theta ) = \cos \theta ; \dfrac{dy}{dt}=\dfrac{d}{dt} (y_{0}+t\sin \theta ) =\sin \theta} \end{eqnarray*} \]
If \(t=0\), then \(x=x_{0}\) and \(y=y_{0}\), and \[ g′ (0)=f_{x}(x_{0},y_{0})\cos \theta +f_{y}(x_{0},y_{0})\sin \theta \underset{\color{#0066A7}{(2)}}{\underset{\color{#0066A7}{\uparrow} }{=}}D_\mathbf{u}f( x_{0},y_{0}) \]
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Solution (a) Since the partial derivatives of \(f\), namely, \[ f_{x}(x,y)=2xy\qquad \hbox{and}\qquad f_{y}(x,y)=x^{2}+2y \]
are continuous, the function \(f\) is differentiable. So, we can use formula (1) with the unit vector \(\mathbf{u}=\cos \dfrac{\pi }{4}\mathbf{i}+\sin \dfrac{\pi }{4}\mathbf{j} =\dfrac{\sqrt{2}}{2}\mathbf{i}+\dfrac{\sqrt{2}}{2 }\mathbf{j}\). Then \[ \begin{eqnarray*} D_{\mathbf{u}}f(x,y)& =&f_{x}(x,y)\cos \theta +f_{y}(x,y)\sin \theta \\ &=& 2xy\cos \dfrac{\pi }{4}+(x^{2}+2y)\sin \dfrac{\pi }{4} \qquad \color{#0066A7}{f_x(x,y)=2xy;} \\ &&\hspace{11.50pc}\color{#0066A7}{f_y (x,y)=x^{2}+2y;\theta =\dfrac{\pi }{4}} \\ &=& \sqrt{2}xy+\dfrac{\sqrt{2}}{2}(x^{2}+2y) \end{eqnarray*} \]
(b) \(D_{\mathbf{u}}f(1,2)=2\sqrt{2}+\dfrac{\sqrt{2}}{2}(1+4)=\dfrac{9\sqrt{2}}{2}\).
(c) When we are at the point \(( 1,2)\) and moving in the direction \(\mathbf{u}=\dfrac{\sqrt{2}}{2}\mathbf{i}+\dfrac{\sqrt{2}}{2} \mathbf{j}\), the function is changing at a rate of approximately 6.364 units per unit length.
Problem 11.
There is another (geometric) interpretation for a directional derivative. Look at Figure 3. If \(P_{0}=(x_{0}, y_{0},0)\) is an interior point in the domain of \(z=\) \(f(x,y)\), then the point \(Q_{0}=( x_{0}, y_{0}, z_{0}) = (x_{0}, y_{0}, f(x_{0}, y_{0}))\) is a point on the surface of \(z\). As we move in the domain of \(f\) along the line \(L\) in the direction of \(\mathbf{u}\), points are traced out on a curve \(C\) that lie on the surface \(z=f( x,y)\). This curve \(C\) is the intersection of the surface and the plane perpendicular to the \(xy\)-plane that contains the line \(L\). It follows that for any point \(P=(x_{0}+t\cos \theta ,y_{0}+t\sin \theta, 0 )\) on \(L\) that is in the domain of \(f\), there is a corresponding point \(Q\) on \(C\). Furthermore, the expression \[ \frac{f(x_{0}+t\cos \theta ,y_{0}+t\sin \theta )-f(x_{0},y_{0})}{t} \qquad t\neq 0 \]
equals the slope of the secant line containing the two points \(Q_{0}\) and \(Q\) on \(C\), and the limit as \(t\rightarrow 0\) is the slope of the tangent line to \(C\) at \(Q_{0}\). This proves the following result.
If \(z=f(x,y)\) is a differentiable function, then the directional derivative \(D_{\mathbf{u}}f(x_{0},y_{0})\) of \(f\) at \((x_{0},y_{0})\) in the direction of \(\mathbf{u}\) equals the slope of the tangent line to the curve \(C\) at the point \(( x_{0}, y_{0}, f(x_{0}, y_{0}))\) on the surface \(z=f( x,y)\), where \(C\) is the intersection of the surface with the plane perpendicular to the \(xy\)-plane and containing the line through \(( x_{0}, y_{0}, 0)\) in the direction \(\mathbf{u}\).
The unit vector \(\mathbf{u}\) in the direction of a given vector is defined in Section 10.3, p. 708.
Find the directional derivative of \(f(x,y)=x\sin y\) at the point \(\left( 2, \dfrac{\pi }{3}\right)\) in the direction of \(\mathbf{a}=3\mathbf{i}+4 \mathbf{j}\). Interpret the result as a slope.
Solution To find a directional derivative of a function \(f\) in the direction of \(\mathbf{a}\), where \(\mathbf{a}\) is a nonzero vector, we must first find the unit vector in the direction of \(\mathbf{a}\). The unit vector \(\mathbf{u}\) in the direction of \(\mathbf{a}\) is \[ \begin{equation*} \mathbf{u}=\frac{\mathbf{a}}{\Vert \mathbf{a}\Vert }=\dfrac{3\mathbf{i}+4 \mathbf{j}}{\sqrt{9+16}}=\frac{3}{5}\mathbf{i}+\frac{4}{5}\mathbf{j} \end{equation*} \]
The partial derivatives of \(f\) \[ f_{x}(x,y)=\sin y\qquad \hbox{and}\qquad f_{y}(x,y)=x\cos y \]
are continuous throughout the plane, so \(f\) is differentiable. Using the unit vector \(\mathbf{u}=\dfrac{3}{5}\mathbf{i}+\dfrac{4}{5}\mathbf{j=}\cos \theta \mathbf{\mathbf{i}+}\sin \theta \mathbf{{j}}\), we find
At the point \(\left( 2,\dfrac{\pi }{3}\right)\), \[ \begin{equation*} D_{\mathbf{u}}f\!\left( 2,\frac{\pi }{3}\right) =\dfrac{3}{5}\sin \dfrac{\pi }{3}+\dfrac{4}{5}\!\left( 2\cos \dfrac{\pi }{3}\right) =\dfrac{3}{5}\!\left( \frac{\sqrt{3}}{2}\right) +\dfrac{8}{5}\!\left(\dfrac{1}{2}\right)=\frac{3\sqrt{3}+8}{10} \end{equation*} \]
The slope of the tangent line to the curve \(C\) that is the intersection of the surface \(f( x,y) =x\sin y\) and the plane perpendicular to the \(xy\)-plane that contains the line through the point \(\left( 2,\dfrac{\pi }{3}, 0\right)\) in the direction \(\mathbf{a}\) is approximately 1.32. See Figure 4.
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Problems 11 and 15.
The directional derivative of a differentiable function \(z=f( x,y)\) at a point \(( x_{0},y_{0})\) in the direction of the unit vector \(\mathbf{u}\) \(=\cos \theta \mathbf{i}+\sin \theta \mathbf{j}\) is given by \[ \begin{equation*} D_{\mathbf{u}}f(x_{0},y_{0})=f_{x}(x_{0},y_{0})\cos \theta +f_{y}(x_{0},y_{0})\sin \theta \end{equation*} \]
We can express \(D_{\mathbf{u}}f(x_{0},y_{0})\) as the dot product of two vectors as follows: \[ \begin{eqnarray*} D_{\mathbf{u}}f(x_{0},y_{0}) &=&f_{x}(x_{0},y_{0})\cos \theta +f_{y}(x_{0},y_{0})\sin \theta \\ &=&[ f_{x}(x_{0},y_{0})\mathbf{i}+f_{y}(x_{0},y_{0})\mathbf{j}]\,{\bf\cdot}\,[ \cos \theta \mathbf{i}+\sin \theta \mathbf{j}] \\ &=&[ f_{x}(x_{0},y_{0})\mathbf{i}+f_{y}(x_{0},y_{0})\mathbf{j}]\, {\bf\cdot}\, \mathbf{u} \end{eqnarray*} \]
The vector \(f_{x}(x_{0},y_{0})\mathbf{i}+f_{y}(x_{0},y_{0})\mathbf{j}\) is called the gradient of \(f\) at \(( x_{0},y_{0})\).
The dot product is discussed in Section 10.4, pp. 715-716.
Let \(z=f(x,y)\) be a differentiable function. The vector \({\bf\nabla}\! f(x,y)\), read “del \(f\),” is called the gradient of \(f\) and is defined as \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ {\bf\nabla}\! f(x,y)=f_{x}(x,y)\mathbf{i}+f_{y}(x,y)\mathbf{j}}} \]
“del \(f\)” is short for “delta \(f\)”; the symbol \({\bf\nabla}\) is an upside down Greek letter delta. In some books, \({\bf\nabla}\! f\) is written as “grad \(f\).” The symbol \({\bf\nabla}\) has no meaning except when it operates on a function \(z = f (x,y)\). So, \({\bf\nabla}\) is referred to as an operator, just as \(\dfrac{d}{dx}\) is an operator indicating “take the derivative of a function of \(x\).”
The directional derivative \(D_{\mathbf{u}}f(x,y)\) of \(f\) can be expressed in terms of the gradient of \(f\).
The dot product of the vector \({\bf\nabla}\! f(x,y)\) and the unit vector \(\mathbf{u}=\cos \theta \mathbf{i}+\sin \theta \mathbf{j}\) is a scalar that is equal to the directional derivative \(D_{\mathbf{u}}f(x,y)\). That is, \[ \begin{equation} \bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ {\bf\nabla}\! f(x,y)\,{\bf\cdot}\, \mathbf{u} =D_{\mathbf{u}}f(x,y) }}\tag{3} \end{equation} \]
\[ \begin{eqnarray*} {\bf\nabla}\! f(x,y)\,{\bf\cdot}\, \mathbf{u} &=& [f_{x}(x,y) \mathbf{i}+f_{y}(x,y)\mathbf{j}] \,{\bf\cdot}\, [ \cos \theta \mathbf{i} +\sin \theta \mathbf{j}] \\ &=& f_{x}(x,y)\cos \theta +f_{y}(x,y)\sin \theta =D_{\mathbf{u}}f(x,y). \end{eqnarray*} \]
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Solution (a) The gradient of \(f\) at \((x,y)\) is \[ {\bf\nabla}\! f(x,y)=f_{x}(x,y)\mathbf{i}+f_{y}(x,y)\mathbf{j}=3x^{2}y \mathbf{i}+x^{3}\mathbf{j} \]
The gradient of \(f\) at \((2,1)\) is \[ {\bf\nabla}\! f(2,1)=12\mathbf{i}+8\mathbf{j} \]
(b) The unit vector \(\mathbf{u}\) from \((2,1)\) to \((3,5)\) is \[ \begin{equation*} \mathbf{u=}\dfrac{( 3-2) \mathbf{i} +( 5-1) \mathbf{j} }{\sqrt{( 3-2) ^{2}+( 5-1) ^{2}}}=\frac{\mathbf{i}+4 \mathbf{j}}{\sqrt{17}} \end{equation*} \]
We use formula (3) for the directional derivative to find \(D_{\mathbf{u} }(2,1).\) \[ \begin{equation*} D_{\mathbf{u}}(2,1)={\bf\nabla\! }f(2,1)\,{\bf\cdot}\, \mathbf{u}=(12\mathbf{i}+8 \mathbf{j})\,{\bf\cdot}\, \frac{\mathbf{i}+4\mathbf{j}}{\sqrt{17}}=\frac{44}{\sqrt{17} } \end{equation*} \]
The directional derivative of \(f\) at \((2,1)\) in the direction of \(\mathbf{u}\) is \(\dfrac{44}{\sqrt{17}}\)
Problem 25.
Let’s look more closely at the directional derivative \(D_{\mathbf{u} }f(x,y)\). \[ \begin{equation} D_{\mathbf{u}}f(x,y)={\bf\nabla\! }f(x,y)\,{\bf\cdot}\, \mathbf{u} \end{equation}\tag{4} \]
The angle between two vectors is discussed in Section 10.4, pp. 716-719.
The directional derivative \(D_{\mathbf{u}}f(x_{0},y_{0})\) is largest when \(\cos \phi =1\). This happens if the angle \(\phi\) between \(\mathbf{u}\) and \({\bf\nabla}\! f\) is \(0\), or equivalently, if \(\mathbf{u}\) and \({\bf \nabla}\! f( x_{0},y_{0})\) have the same direction. In this case, the maximum value of the directional derivative is \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ \hbox{Maximum value of } D_{\mathbf{u}}f(x_{0},y_{0})=\left\Vert {\bf \nabla\! }f(x_{0},y_{0})\right\Vert }} \]
Similarly, the minimum value of \(D_{\mathbf{u}}f(x_{0},y_{0})\) occurs when \(\cos \phi =-1\), that is, when \(\phi =\pi\). This happens when \(\mathbf{u}\) and \({\bf\nabla}\! f\) are opposite in direction. The minimum value of the directional derivative is \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ \hbox{Minimum value of } D_{\mathbf{u}}f(x_{0},y_{0})=-\left\Vert {\bf \nabla\! }f(x_{0},y_{0})\right\Vert }} \]
Suppose the function \(z=f(x,y)\) is differentiable at \((x_{0},y_{0})\).
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Solution (a) We begin by finding the gradient of \(f\) at \((1,-2)\). \[ \begin{array}{rcl@{\qquad}l} {\bf\nabla\! }f(x,y) &=&(2x-y)\mathbf{i}+(2y-x)\mathbf{j} & \color{#0066A7}{{\bf\nabla}\! f(x,y)=f_{x}(x,y) \mathbf{i}+f_{y}(x,y)\mathbf{j}} \\ {\bf\nabla\! }f(1,-2) &=&4\mathbf{i}-5\mathbf{j} & \color{#0066A7}{{x=1; y=-2}} \end{array} \]
The direction \(\mathbf{u}\) for which \(D_{\mathbf{u}}f(1,-2)\) is maximum occurs when \({\bf\nabla}\! f\) and the unit vector \(\mathbf{u}\) have the same direction. That is, the directional derivative is a maximum when the direction is \(\mathbf{u}=\dfrac{4\sqrt{41}}{41}\mathbf{i}-\dfrac{5\sqrt{41}}{ 41}\mathbf{j}\).
(b) The maximum value of the directional derivative at \((1,-2)\) equals the magnitude of the gradient, namely \[ \Vert {\bf\nabla}\! f(1,-2)\Vert =\sqrt{16+25}=\sqrt{41} \]
Problem 35.
The directional derivative \(D_{\mathbf{u}}f(x_{0},y_{0})\) equals the rate of change of \(z=\) \(f( x,y)\) at \((x_{0},y_{0})\) in the direction of \(\mathbf{u}\). When \(\mathbf{u}\) has the same direction as \({\bf\nabla}\! f(x_{0},y_{0})\), then the rate of change of \(f\) at \((x_{0},y_{0})\) is a maximum. It follows that \(f(x,y)\) will increase most rapidly in this direction.
Suppose \(z=f(x,y)\) is differentiable at \((x_{0},y_{0})\) and \({\bf\nabla}\! f (x_{0},y_{0}) \neq \mathbf{0}\).
The second statement is a consequence of (5). If \(\phi\) is the angle between \(\mathbf{u}\) and \({\bf\nabla}\! f\), the rate of change of \(z\) in the direction of \(\mathbf{u}\) is \(0\) when \[ \begin{equation*} D_{\mathbf{u}}f(x_{0},y_{0})={\bf\nabla\! }f\,{\bf\cdot}\, \mathbf{u}=\Vert {\bf \nabla\! }f(x_{0},y_{0})\Vert \cos \phi =0 \qquad 0\leq \phi \leq \pi \end{equation*} \]
If \({\bf\nabla}\! f(x_{0},y_{0})\neq \mathbf{0}\), then \(\cos \phi =0\), or equivalently, \(\phi =\dfrac{\pi }{2}\). In other words, the rate of change of \(z\) is \(0\) when the direction of \(\mathbf{u}\) is orthogonal to \({\bf\nabla}\! f(x_{0},y_{0})\).
A metal plate is placed on the \(xy\)-plane in such a way that the temperature \(T\) in degrees Celsius at any point \(P=(x,y)\) is inversely proportional to the distance of \(P\) from \((0,0)\). Suppose the temperature of the plate at the point \((-3,4)\) equals \({50^{\circ}{\rm C}}\).
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Solution (a) The temperature \(T\) at any point \((x,y)\) is inversely proportional to the distance of \(( x,y)\) from the origin \((0,0)\). We can model \(T=T( x,y)\) as \[ T(x,y)=\dfrac{k}{\sqrt{x^{2}+y^{2}}} \]
where \(k\) is the constant of proportionality. Since \(T=50^{\circ}{\rm C}\) when \((x,y)=(-3,4)\), then \[ k=T\sqrt{x^{2}+y^{2}}=50\sqrt{( -3) ^{2}+4^{2}}=50(5)=250 \]
So, \(T=T( x,y) =\dfrac{250}{\sqrt{x^{2}+y^{2}}}\).
(b) The gradient of \(T=T( x,y) =\dfrac{250}{\sqrt{ x^{2}+y^{2}}}\) is \[ {\bf\nabla }T(x,y)=T_{x}(x,y)\mathbf{i}+T_{y}(x,y)\mathbf{j}=-\frac{250x }{(x^{2}+y^{2})^{3/2}}\mathbf{i}-\frac{250y}{(x^{2}+y^{2})^{3/2}}\mathbf{ j} \]
At \(( -3,4)\), \[ {\bf\nabla }T(-3,4)=-\frac{250 ( -3) }{ [ ( -3) ^{2}+4^{2}] ^{3/2}}\mathbf{i}-\frac{250 ( 4) }{ [ ( -3) ^{2}+4^{2}] ^{3/2}}\mathbf{j}=\frac{750}{125} \mathbf{i}-\frac{1000}{125}\mathbf{j}=6\mathbf{i}-8\mathbf{j} \]
(c) The temperature increases most rapidly in the direction \({\bf\nabla} T(-3,4)=6\mathbf{i}-8\mathbf{j}\).
(d) The temperature decreases most rapidly in the direction \(-{\bf\nabla }T(-3,4)=-6\mathbf{i}+8\mathbf{j}\).
(e) The rate of change in \(T\) at \((-3,4)\) equals \(0\) for directions orthogonal to \({\bf\nabla} T(-3,4)=6\mathbf{i}-8\mathbf{j}\). That is, the rate of change in \(T\) is \(0\) in either of the two directions orthogonal to \(6\mathbf{i}-8\mathbf{j}\), namely \(\pm ( 8\mathbf{i}+6 \mathbf{j})\).
Level curves are discussed in Section 12.1, pp. 812-814.
Figure 5 shows the graph of the surface \(T=T( x,y)\).
Problem 47.
The grade of a mountain is a measure of its steepness. The name gradient given to \({\bf\nabla}\! f\) means the direction of steepest ascent.
Suppose the surface \(z=f(x,y)\) represents a mountain whose elevation above sea level is \(z\). See Figure 6(a). The level curves of \(f\) shown in Figure 6(b) correspond to contour lines along which the elevation remains fixed. So along the level curves, the value of \(z\) does not change. The elevation increases (or decreases) most rapidly in directions perpendicular to the level curves. In other words, the most direct (but steepest) route to the top of the mountain is in the direction of \({\bf\nabla}\! f\), which is orthogonal to the level curves. The shortest route down the mountain is in the direction of \(- {\bf\nabla}\!f\), which is also perpendicular to the level curves. A stream of water flows this way down the mountain. As water moves from one level curve to another, the gradient changes, giving the water a new direction. See Figure 7.
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Suppose the function \(z=f(x,y)\) is differentiable at a point \(P_{0}=(x_{0},y_{0})\). If \({\bf\nabla}\! f(x_{0},y_{0})\neq \mathbf{0}\), then \({\bf\nabla}\! f(x_{0},y_{0})\) is normal to the level curve of \(f\) at \(P_{0}\).
A normal vector to a curve at a point \(P\) is defined as a vector with initial point at \(P\) and orthogonal (perpendicular) to the tangent line to the curve at \(P\).
Let \(f(x,y)=k\) be the level curve through \(P_{0}\). Suppose this level curve is represented parametrically by \(x=x(t)\) and \(y=y(t)\), with \(x_{0}=x(t_{0})\) and \(y_{0}=y(t_{0})\). Then \[ \begin{equation*} f( x(t),y(t)) =k \end{equation*} \]
Differentiating \(f( x(t),y(t))\) with respect to \(t\), we get \[ \begin{equation*} f_{x}( x(t),y(t))\, x′ (t)+f_{y}( x(t),y(t))\, y′ (t)=0 \qquad \color{#0066A7}{\hbox{Use Chain Rule I.}} \end{equation*} \]
or, equivalently, \[ \begin{equation*} {\bf\nabla\! }f(x,y)\,{\bf\cdot}\, \lbrack x′ (t)\mathbf{i}+y′ (t) \mathbf{j}]=0 \end{equation*} \]
Since \(x′ (t) \mathbf{i}+y′ (t) \mathbf{j}\) is tangent to the level curve, the vector \({\bf\nabla\! }f( x,y)\) is normal to the level curve. In particular, when \(t=t_{0}\), \({\bf\nabla}\! f(x_{0},y_{0})\) is normal to the level curve of \(f\) at \((x_{0},y_{0})\).
For the function \(f(x,y)=\sqrt{x^{2}+y^{2}}\), graph the level curve containing the point \((3,4)\) and graph the gradient \({\bf\nabla\! }f(x,y)\) at this point.
Solution See Figure 8(a). The graph of the equation \(z=\sqrt{x^{2}+y^{2}}\) is the upper half of a circular cone whose traces are circles. So, the level curves are concentric circles centered at \(( 0,0)\). Because \(f(3,4)=\sqrt{9+16}=5\), the level curve through \((3,4)\) is the circle \(x^{2}+y^{2}=25\). Since \[ \begin{equation*} {\bf\nabla}\! f(x,y)=\frac{x}{\sqrt{x^{2}+y^{2}}}\mathbf{i}+\frac{y}{\sqrt{ x^{2}+y^{2}}}\mathbf{j} \end{equation*} \]
the gradient at \((3,4)\) is \[ \begin{equation*} {\bf\nabla}\! f(3,4)=\frac{3}{5}\mathbf{i}+\frac{4}{5}\mathbf{j} \end{equation*} \]
This vector is orthogonal to the level curve \(x^{2}+y^{2}=25\), as shown in Figure 8(b).
Problem 45.
871
The concepts of directional derivative and gradient can be extended to a function \(w=f(x,y,z)\) of three variables.
The directional derivative \(D_{\mathbf{u} }f(x_{0},y_{0},z_{0})\) of a function \(w=f(x,y,z)\) at \((x_{0},y_{0},z_{0})\) in the direction of a unit vector \(\mathbf{u=}\) \(\cos \alpha \mathbf{i} +\cos \beta \mathbf{j}+\cos \gamma \mathbf{k}\) is given by \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ D_{\mathbf{u}}f(x_{0},y_{0},z_{0})=\lim\limits_{t\rightarrow 0} \dfrac{f(x_{0}+t\cos \alpha ,y_{0}+t\cos \beta ,z_{0}+t\cos \gamma )-f(x_{0},y_{0},z_{0})}{t} }} \]
provided the limit exists.
If the function \(w= f(x,y,z)\) is differentiable, then the directional derivative of \(f\) in the direction of \(\mathbf{u}=\cos \alpha \mathbf{i} +\cos \beta \mathbf{j}+\cos \gamma \mathbf{k}\) equals \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ D_{\mathbf{u}}f(x_{0},y_{0},z_{0})=f_{x}(x_{0},y_{0},z_{0})\cos \alpha +f_{y}(x_{0},y_{0},z_{0})\cos \beta +f_{z}(x_{0},y_{0},z_{0})\cos \gamma }} \]
As with functions of two variables, the directional derivative \(D_{\mathbf{u} } f(x_{0}, y_{0}, z_{0})\) equals the rate of change of \(f\) at \((x_{0}, y_{0}, z_{0})\) in the direction of \(\mathbf{u}\).
Let \(w = f(x,y,z)\) be a differentiable function. Then the gradient of \(f\) at \((x_{0},y_{0},z_{0})\) is the vector \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ {\bf\nabla}\! f(x_{0},y_{0},z_{0})=f_{x}(x_{0},y_{0},z_{0})\mathbf{i} +f_{y}(x_{0},y_{0},z_{0})\mathbf{j}+f_{z}(x_{0},y_{0},z_{0})\mathbf{k} }} \]
Then, as for functions of two variables, the directional derivative of \(f\) at \(\left( x_{0},y_{0},z_{0}\right)\) in the direction of \(\mathbf{u}\) can be found using the gradient as follows: \[\bbox[5px, border:1px solid black, #F9F7ED]{\bbox[#FAF8ED]{ D_{\mathbf{u}}f(x_{0},y_{0},z_{0})= \bf\nabla\! f(x_{0},y_{0},z_{0})\,{\bf\cdot}\, \mathbf{u}=\left\Vert {\bf\nabla\! } f(x_{0},y_{0},z_{0})\right\Vert \cos \phi }} \]
where \(\phi\) is the angle between \({\bf\nabla}\! f(x_{0},y_{0},z_{0})\) and \(\mathbf{u}\).
As with functions of two variables, the value of \(f\) increases most rapidly in the direction of the gradient \({\bf\nabla\! }f(x_{0},y_{0},z_{0})\), and decreases most rapidly in the direction of \(-{\bf\nabla\! } f(x_{0},y_{0},z_{0})\).
For example, suppose \(T=T(x,y,z)\) is the temperature of a homogeneous object at the point \((x,y,z)\). At the point \((x_{0},y_{0},z_{0})\) on the object, heat will flow in the direction of greatest decrease in temperature, namely in the direction of \(-{\bf\nabla }T(x_{0},y_{0},z_{0})\). This direction of greatest heat transfer is normal to the level surface through \((x_{0},y_{0},z_{0})\).
Suppose the function \(w = f(x, y, z)\) is differentiable at a point \(P_{0}=(x_{0}, y_{0}, z_{0})\). If \({\bf\nabla\! }f(x_{0}, y_{0}, z_{0})\neq \mathbf{0}\), the gradient \({\bf\nabla\! }f(x_{0}, y_{0}, z_{0})\) is normal to the level surface of \(f\) through \(P_{0}\).
You are asked to prove this in Problem 76.