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Find the area of the surface \(x^{2}-2 y-2 z=0\) that lies above the triangle bounded by the lines \(x=2, y=0,\) and \(y=3 x\) in the \(x y\) -plane.

Short Answer

Expert verified
The surface area is \(6\sqrt{6} - 2\sqrt{2}\).

Step by step solution

01

Identify the Surface and Region

The given surface is defined by the equation \(x^{2} - 2y - 2z = 0\). Therefore, the value of \(z\) can be expressed as \(z = \frac{x^2}{2} - y\). The region in the \(xy\)-plane above which we need to find the surface area is a triangle bounded by the lines \(x=2\), \(y = 0\), and \(y = 3x\).
02

Determine the Triangle's Vertices

Let's find the vertices of the triangular region:- The line \(x = 2\) intersects \(y = 3x\) at the point \((2, 6)\).- The line \(y = 0\) intersects \(x = 2\) at the point \((2, 0)\).- The line \(y = 3x\) intersects \(y = 0\) at the point \((0, 0)\).Thus, the triangle's vertices are \((0, 0), (2, 0), (2, 6)\).
03

Define the Integral for Surface Area

The formula for surface area of a function \(z = f(x,y)\) over a region \(R\) in the \(xy\)-plane is given by \[\iint_R \sqrt{1 + \left(\frac{\partial f}{\partial x}\right)^2 + \left(\frac{\partial f}{\partial y}\right)^2} \, dx \, dy\].For \(f(x, y) = \frac{x^2}{2} - y\), we need the partial derivatives as follows:- \(\frac{\partial f}{\partial x} = x\)- \(\frac{\partial f}{\partial y} = -1\).Therefore, the integrand becomes \(\sqrt{1 + x^2 + 1} = \sqrt{x^2 + 2}\).
04

Set the Integration Bounds

The triangle in the \(xy\)-plane is bounded by:- \(x\) ranging from 0 to 2,- \(y\) ranging from 0 to \(3x\).
05

Compute the Double Integral

We compute the double integral \[\int_{0}^{2} \int_{0}^{3x} \sqrt{x^2 + 2} \, dy \, dx\].Integrating with respect to \(y\) gives:\[\int_{0}^{3x} \sqrt{x^2 + 2} \, dy = \sqrt{x^2 + 2} \cdot y \bigg|_{0}^{3x} = 3x\sqrt{x^2 + 2}\].
06

Finish the Integration Over x

The integral simplifies to \[\int_{0}^{2} 3x\sqrt{x^2 + 2} \, dx\].Using substitution (let \(u = x^2 + 2\), thus \(du = 2x \, dx\)), we transform:\[\int 3x\sqrt{x^2 + 2} \, dx = \frac{3}{2} \int \sqrt{u} \, du\].With limits changing from \(x = 0\) to \(x = 2\), \(u\) ranges from 2 to 6.The integral is solved as:\[\frac{3}{2} \left( \frac{2}{3} u^{3/2} \right) \bigg|_{2}^{6} = u^{3/2} \bigg|_{2}^{6}\]Calculating gives \( (6^{3/2} - 2^{3/2}) = (6\sqrt{6} - 2\sqrt{2})\), which simplifies the final result to the surface area.

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Key Concepts

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

Surface Integral
A surface integral is a way to extend the concept of integration to surfaces. Unlike a regular integral, which moves over a line or area, a surface integral spans a two-dimensional surface. Imagine draping a sheet over some terrain; the surface integral calculates how that sheet behaves, factoring in the curves and slopes of the land beneath.

In the context of the problem, the surface integral helps us find the total area of a surface over a specific region. This surface is defined in the 3D space, determined by the given equation of the surface and the corresponding boundaries on the xy-plane. Here, we utilize the formula:
\[\iint_R \sqrt{1 + \left(\frac{\partial f}{\partial x}\right)^2 + \left(\frac{\partial f}{\partial y}\right)^2} \, dx \, dy\]
This formula takes into account the two-dimensional "bumpiness" or "height differences" of the surface by incorporating the partial derivatives of the surface function. Calculating the surface integral involves determining these partial derivatives and applying them over the designated region "R."
Double Integral
A double integral is an extension of a regular integral that calculates over an area in a plane, typically the xy-plane. When using a double integral, we consider not just the accumulation in a single direction but across an entire plane. This is particularly useful for calculating volumes beneath a surface or areas over a region.

In this exercise, we set up the double integral to determine the surface area over the triangular region stated in the problem. We defined limits for both x and y based on the triangle's bounds. Specifically:
  • For x: From 0 to 2
  • For y: From 0 to 3x
These bounds define the area over which the double integral operates, gathering all the infinitesimally small contributions of area from within the triangular region. Through evaluating the double integral:
\[\int_{0}^{2} \int_{0}^{3x} \sqrt{x^2 + 2} \, dy \, dx\]
We find the total surface area by accumulating these contributions over the entire specified region.
Partial Derivatives
Partial derivatives are a foundational concept in multivariable calculus. They measure how a multi-variable function changes as one of its variables changes, while the others remain constant. It’s like determining the slope of a mountain path when you only adjust your elevation or your north-south position without moving east-west.

In surface area calculations, partial derivatives provide the necessary rates of change along each primary axis in the xy-plane. They refine our understanding of the surface's slope and how much more "area" that slope adds. For our surface defined by the equation \(z = \frac{x^2}{2} - y\), we find the partial derivatives:
  • With respect to x: \(\frac{\partial f}{\partial x} = x\)
  • With respect to y: \(\frac{\partial f}{\partial y} = -1\)
These derivatives are then used in the surface integral formula to accurately account for the surface’s curvature over the triangular region.
Substitution Method in Calculus
The substitution method is a classical technique in calculus for simplifying the evaluation of integrals. It involves substituting an expression with another variable, making the integral easier to solve. This is akin to changing the units in a problem to ones that make arithmetic straightforward.

In the final steps of integration in this problem, we used substitution to simplify the integral
\[\int 3x\sqrt{x^2 + 2} \, dx\]
After letting \(u = x^2 + 2\), we derived \(du = 2x \, dx\), allowing the integral to be rewritten in terms of \(u\). This change streamlined the problem, freeing us from complex terms in x and turning it into:
\[\frac{3}{2} \int \sqrt{u} \, du\]
By replacing the bounds to accommodate the new variable, the integral could be easily evaluated. This useful trick reaffirmed the power of substitution in tackling otherwise complicated integrals by shifting to simpler forms.

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Most popular questions from this chapter

Green's Theorem and Laplace's equation Assuming that all the necessary derivatives exist and are continuous, show that if \(f(x, y)\) satisfies the Laplace equation $$ \frac{\partial^{2} f}{\partial x^{2}}+\frac{\partial^{2} f}{\partial y^{2}}=0 $$ then $$ \oint_{\mathcal{C}} \frac{\partial f}{\partial y} d x-\frac{\partial f}{\partial x} d y=0 $$ for all closed curves \(C\) to which Green's Theorem applies. (The converse is also true: If the line integral is always zero, then \(f\) satisfies the Laplace equation.)

Calculating Area with Green's Theorem If a simple closed curve C in the plane and the region \(R\) it encloses satisfy the hypotheses of Green's Theorem, the area of \(R\) is given by Green's Theorem Area Formula Area of \(R=\frac{1}{2} \oint_{c} x d y-y d x\) The reason is that, by Equation (4) run backward, Area of \(R=\iint_{k} d y d x=\iint_{k}\left(\frac{1}{2}+\frac{1}{2}\right) d y d x\) $$=\oint_{c} \frac{1}{2} x d y-\frac{1}{2} y d x$$ Use the Green's Theorem area formula given above to find the areas of the regions enclosed by the curves in Exercises \(31-34\) The circle \(\mathbf{r}(t)=(a \cos t) \mathbf{i}+(a \sin t) \mathbf{j}, \quad 0 \leq t \leq 2 \pi\)

Conservation of mass \(\quad\) Let \(\mathbf{v}(t, x, y, z)\) be a continuously differentiable vector field over the region \(D\) in space, and let \(p(t, x,\) \(y, z)\) be a continuously differentiable scalar function. The variable t represents the time domain. The Law of Conservation of Mass asserts that $$\frac{d}{d t} \iiint_{D} p(t, x, y, z) d V=-\iint_{S} p \mathbf{v} \cdot \mathbf{n} d \sigma,$$ where \(S\) is the surface enclosing \(D\). a. Give a physical interpretation of the conservation of mass law if \(\mathbf{v}\) is a velocity flow field and \(p\) represents the density of the fluid at point \((x, y, z)\) at time \(t\) b. Use the Divergence Theorem and Leibniz's Rule, $$\frac{d}{d t} \iiint_{D} p(t, x, y, z) d V=\iiint_{D} \frac{\partial p}{\partial t} d V,$$ to show that the Law of Conservation of Mass is equivalent to the continuity equation, $$\nabla \cdot p \mathbf{v}+\frac{\partial p}{\partial t}=0.$$ (In the first term \(\nabla \cdot p \mathbf{v},\) the variable \(t\) is held fixed, and in the second term \(\partial p / \partial t,\) it is assumed that the point \((x, y, z)\) in \(D\) is held fixed.)

Find the area of the surface \(2 x^{3 / 2}+2 y^{3 / 2}-3 z=0\) above the square \(R: 0 \leq x \leq 1,0 \leq y \leq 1,\) in the \(x y\) -plane.

Path of least work You have been asked to find the path along which a force field \(\mathbf{F}\) will perform the least work in moving a particle between two locations. A quick calculation on your part shows \(\mathbf{F}\) to be conservative. How should you respond? Give reasons for your answer.

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