/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 28 The tangent plane at a point \(P... [FREE SOLUTION] | 91Ó°ÊÓ

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The tangent plane at a point \(P_{0}\left(f\left(u_{0}, v_{0}\right), g\left(u_{0}, v_{0}\right), h\left(u_{0}, v_{0}\right)\right)\) on a parametrized surface \(\mathbf{r}(u, \boldsymbol{v})=f(u, v) \mathbf{i}+g(u, v) \mathbf{j}+h(u, v) \mathbf{k}\) is the plane through \(P_{0}\) normal to the vector \(\mathbf{r}_{u}\left(u_{0}, v_{0}\right) \times \mathbf{r}_{v}\left(u_{0}, v_{0}\right),\) the cross product of the tangent vectors \(\mathbf{r}_{u}\left(u_{0}, v_{0}\right)\) and \(\mathbf{r}_{v}\left(u_{0}, v_{0}\right)\) at \(P_{0}\) . Find an equation for the plane tangent to the surface at \(P_{0} .\) Then find a Cartesian equation for the surface and sketch the surface and tangent plane together. Hemisphere The hemisphere surface \(\mathbf{r}(\phi, \theta)=(4 \sin \phi \cos \theta) \mathbf{i}\) \(+(4 \sin \phi \sin \theta) \mathbf{j}+(4 \cos \phi) \mathbf{k}, 0 \leq \phi \leq \pi / 2,0 \leq \theta \leq 2 \pi\) at the point \(P_{0}(\sqrt{2}, \sqrt{2}, 2 \sqrt{3})\) corresponding to \((\phi, \theta)=\) \((\pi / 6, \pi / 4)\)

Short Answer

Expert verified
The tangent plane equation is \(4\sqrt{3}(x + y) + 4z = 16\). The hemisphere's Cartesian equation is \(x^2 + y^2 + z^2 = 16\).

Step by step solution

01

Identify Components and Parameters

The surface is given by \(\mathbf{r}(\phi, \theta) = (4 \sin \phi \cos \theta) \mathbf{i} + (4 \sin \phi \sin \theta) \mathbf{j} + (4 \cos \phi) \mathbf{k}\). With parameters \(\phi\) and \(\theta\), we identify the point \(P_0(\sqrt{2}, \sqrt{2}, 2\sqrt{3})\) corresponds to \((\phi, \theta) = (\pi/6, \pi/4)\).
02

Calculate Partial Derivatives

Compute \(\mathbf{r}_{\phi}\) and \(\mathbf{r}_{\theta}\):\[\mathbf{r}_{\phi} = \left(4 \cos \phi \cos \theta\right) \mathbf{i} + \left(4 \cos \phi \sin \theta\right) \mathbf{j} - 4 \sin \phi \mathbf{k}\] \[\mathbf{r}_{\theta} = \left(-4 \sin \phi \sin \theta\right) \mathbf{i} + \left(4 \sin \phi \cos \theta\right) \mathbf{j} + 0 \mathbf{k}\].
03

Find the Normal Vector

Calculate the cross product \(\mathbf{r}_{\phi} \times \mathbf{r}_{\theta}\):\[\mathbf{r}_{\phi}(\pi/6, \pi/4) = \left(\sqrt{2} \right) \mathbf{i} + \left(\sqrt{2} \right) \mathbf{j} - 2 \sqrt{3} \mathbf{k}\] \[\mathbf{r}_{\theta}(\pi/6, \pi/4) = -2 \mathbf{i} + 2 \mathbf{j}\]The cross product is \[\mathbf{n} = \mathbf{r}_{\phi} \times \mathbf{r}_{\theta} = (4 \sqrt{3}) \mathbf{i} + (4 \sqrt{3}) \mathbf{j} + (4) \mathbf{k}\].
04

Write the Tangent Plane Equation

Using \(\mathbf{n} = (4 \sqrt{3}, 4 \sqrt{3}, 4)\) and point \(P_0 (\sqrt{2}, \sqrt{2}, 2\sqrt{3})\), the tangent plane equation is \[4\sqrt{3}(x - \sqrt{2}) + 4\sqrt{3}(y - \sqrt{2}) + 4(z - 2\sqrt{3}) = 0\].
05

Simplify Tangent Plane Equation

Simplifying the equation:\[4\sqrt{3}x + 4\sqrt{3}y + 4z - 16 = 0\].
06

Convert Parametric Surface to Cartesian Equation

Converting hemispherical parametric equations \(x = 4 \sin \phi \cos \theta\), \(y = 4 \sin \phi \sin \theta\), \(z = 4 \cos \phi\) by squaring and adding:\[x^2 + y^2 + z^2 = 16\].
07

Sketch the Surface and Tangent Plane

The hemisphere \(x^2 + y^2 + z^2 = 16\) lives above the xy-plane (\(z \geq 0\)). The tangent plane "touches" the hemisphere at \((\sqrt{2}, \sqrt{2}, 2\sqrt{3})\). Sketch the hemisphere as the upper half of a sphere, and the plane intersecting the hemisphere at its tangent point.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Parametrized Surface
A parametrized surface uses parameters, typically denoted as \( u \) and \( v \), to describe a surface in three-dimensional space. In this context, these parameters help express complex surfaces with simple, mathematical functions. The surface might be presented as a vector function \( \mathbf{r}(u, v) = f(u, v) \mathbf{i} + g(u, v) \mathbf{j} + h(u, v) \mathbf{k} \), which implies that the surface is traced by varying \( u \) and \( v \).

For our hemisphere example, the parameters \( \phi \) and \( \theta \) are specifically chosen to exploit spherical coordinates, making it easier to express a hemisphere. These types of surfaces are powerful in that they allow us to manipulate and explore geometrically complex shapes through simple mathematical tools.

With parametrized surfaces, you can:
  • Describe curved surfaces with simple equations.
  • Calculate tangent vectors and then normal vectors.
  • Use parameters to dynamically model surface behaviors.
Cross Product
The cross product is a vector operation that takes two vectors in three-dimensional space and produces another vector that is perpendicular to both of the original vectors. This new vector is often called the normal vector, and its length corresponds to the area of the parallelogram formed by the two vectors.

In the context of finding a tangent plane, we start with tangent vectors \( \mathbf{r}_{u} \) and \( \mathbf{r}_{v} \) derived from the partial derivatives of the surface function. The cross product \( \mathbf{r}_{u} \times \mathbf{r}_{v} \) gives us the normal vector - a crucial component used to define the plane that is tangent to our surface at a specific point.

Key properties of the cross product include:
  • Your resulting vector is orthogonal to both original vectors.
  • Allows calculation of planes and determining orientations.
  • Vector has a magnitude that helps interpret spatial interactions.
Cartesian Equation
A Cartesian equation is an equation that relates \( x \), \( y \), and \( z \) coordinates directly, typically using algebra without involving any parameters. Once a parametrized surface is defined, converting it to a Cartesian form helps visualize the surface in regular coordinate operations.

In the exercise, we converted the parameterized hemisphere equations \( x = 4 \sin \phi \cos \theta \), \( y = 4 \sin \phi \sin \theta \), and \( z = 4 \cos \phi \) into the Cartesian equation \( x^2 + y^2 + z^2 = 16 \). This is achieved by using trigonometric identities to eliminate parameters, showing the hemisphere as part of a sphere in a clearer algebraic form.

Benefits of Cartesian equations include:
  • Easier visualization and graph plotting.
  • Simplified algebraic manipulation for calculations.
  • Direct interpretation without needing parameter adjustments.
Partial Derivatives
Partial derivatives are essential in multivariable calculus, allowing us to understand changes along specific dimensions while treating other variables as constants. They are especially prevalent in calculating the slope of surfaces.

For a parametrized surface \( \mathbf{r}(u, v) = f(u, v) \mathbf{i} + g(u, v) \mathbf{j} + h(u, v) \mathbf{k} \), partial derivatives \( \mathbf{r}_{u} \) and \( \mathbf{r}_{v} \) give us the tangent vectors at any point \( (u, v) \) on the surface. These tangent vectors demonstrate how the surface changes along each of the parameter directions.

In practice, understanding partial derivatives assists with:
  • Finding and analyzing tangent planes.
  • Determining surface behavior and shape.
  • Solving optimization problems in higher dimensions.

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Most popular questions from this chapter

In Exercises \(43-46,\) use a CAS and Green's Theorem to find the counterclockwise circulation of the field \(F\) around the simple closed curve C. Perform the following CAS steps. $$\begin{array}{l}{\text { a. Plot } C \text { in the } x y \text { -plane. }} \\\ {\text { b. Determine the integrand }(\partial N / \partial x)-(\partial M / \partial y) \text { for the tangen- }} \\ {\text { tial form of Green's Theorem. }} \\ {\text { c. Determine the (double integral) limits of integration from }} \\ {\text { your plot in part (a) and evaluate the curl integral for the }} \\ {\text { circulation. }}\end{array}$$ $$\mathbf{F}=(2 x-y) \mathbf{i}+(x+3 y) \mathbf{j}, \quad C : \text { The ellipse } x^{2}+4 y^{2}=4$$

a. A torus of revolution (doughnut) is obtained by rotating a circle \(C\) in the \(x z\) -plane about the \(z\) -axis in space. (See the accompanying figure.) If \(C\) has radius \(r>0\) and center \((R, 0,0),\) show that a parametrization of the torus is $$\begin{aligned} \mathbf{r}(u, v)=&((R+r \cos u) \cos v) \mathbf{i} \\\ &+((R+r \cos u) \sin v) \mathbf{j}+(r \sin u) \mathbf{k} \end{aligned}$$ where \(0 \leq u \leq 2 \pi\) and \(0 \leq v \leq 2 \pi\) are the angles in the figure. b. Show that the surface area of the torus is \(A=4 \pi^{2} R r\)

Regions with many holes Green's Theorem holds for a region \(R\) with any finite number of holes as long as the bounding curves are smooth, simple, and closed and we integrate over each component of the boundary in the direction that keeps \(R\) on our immediate left as we go along (see accompanying figure). $$\begin{array}{l}{\text { a. Let } f(x, y)=\ln \left(x^{2}+y^{2}\right) \text { and let } C \text { be the circle }} \\ {x^{2}+y^{2}=a^{2} . \text { Evaluate the flux integral }}\end{array}$$ $$\oint_{C} \nabla f \cdot \mathbf{n} d s$$ b. Let \(K\) be an arbitrary smooth, simple closed curve in the plane that does not pass through \((0,0) .\) Use Green's Theorem to show that $$\oint_{K} \nabla f \cdot \mathbf{n} d s$$ has two possible values, depending on whether \((0,0)\) lies inside \(K\) or outside \(K .\)

Find the outward flux of the field \(\mathbf{F}=2 x y \mathbf{i}+2 y z \mathbf{j}+2 x z \mathbf{k}\) across the surface of the cube cut from the first octant by the planes \(x=a, y=a, z=a.\)

(Continuation of Exercise \(34 . )\) Find a Cartesian equation for the plane tangent to the hyperboloid \(x^{2}+y^{2}-z^{2}=25\) at the point \(\left(x_{0}, y_{0}, 0\right),\) where \(x_{0}^{2}+y_{0}^{2}=25\)

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