Section 2.3

Integral Calculus

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Problem 2.3.1

What is the volume enclosed by the ellipsoid

x2a2+y2b2+z2c2=1 ? \frac{x^2}{a^2} + \frac{y^2}{b^2} + \frac{z^2}{c^2} = 1 \, ?
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Problem 2.3.2

Evaluate

∬Ae−x2−y2 dx dy, \iint _{\mathcal{A}} e^{-x^2-y^2} \, dx \, dy,

where A={(x,y)∈R2∣x2+y2≤1}\mathcal{A} = \left\{ (x,y) \in \mathbb {R}^{2} \mid x^2+y^2 \leq 1\right\}.

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Problem 2.3.3

Given the fact that ∫−∞∞e−x2 dx=π\displaystyle \int_{-\infty }^{\infty } e^{-x^2} \, dx = \sqrt{\pi }, evaluate the integral

I=∫−∞∞∫−∞∞e−(x2+(y−x)2+y2) dx dy. I = \int _{-\infty }^{\infty } \int _{-\infty }^{\infty } e^{-(x^2+(y-x)^2+y^2)} \, dx \, dy.
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Problem 2.3.4

Evaluate

∬R(x3−3xy2) dx dy, \iint _{\mathcal{R}} (x^3 - 3xy^2) \, dx \, dy,

where

R={(x,y)∈R2∣(x+1)2+y2≤9, (x−1)2+y2≥1}. \mathcal{R} = \left\{ (x,y) \in \mathbb {R}^{2} \mid (x+1)^2+y^2 \leq 9, \ (x-1)^2+y^2 \geq 1\right\} .
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Problem 2.3.5

Let φ(x,y)\varphi (x,y) be a function with continuous second order partial derivatives such that

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(1)

φxx+φyy+φx=0\varphi_{xx} + \varphi_{yy} + \varphi_x = 0 in the punctured plane R2∖{0}\mathbb {R}^{2} \setminus \left\{ 0\right\},

(2)

rφx→x2πrr\varphi_x \to \dfrac {x}{2\pi r} and rφy→y2πrr\varphi_y \to \dfrac {y}{2\pi r} as r=x2+y2→0r = \sqrt{x^2+y^2} \to 0.

Let CRC_R be the circle x2+y2=R2x^2+y^2=R^2. Show that the line integral

∫CRex(−φy dx+φx dy) \int _{C_R} e^x(-\varphi _y \, dx + \varphi _x \, dy)

is independent of RR, and evaluate it.

Problem 2.3.6

Let S={(x,y,z)∈R3∣x2+y2+z2=1}S = \left\{ (x,y,z) \in \mathbb {R}^{3} \mid x^2+y^2+z^2=1\right\} denote the unit sphere in R3\mathbb {R}^{3}. Evaluate the surface integral over SS:

∬S(x2+y+z) dA. \iint _S (x^2+y+z) \, dA.
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Problem 2.3.7

Let i→\overrightarrow {i}, j→\overrightarrow {j}, and k→\overrightarrow {k} be the usual unit vectors in R3\mathbb {R}^{3}. Let F→\overrightarrow {F} denote the vector field

(x2+y−4)i→+3xyj→+(2xz+z2)k→. (x^2+y-4)\overrightarrow {i} + 3xy\overrightarrow {j} + (2xz+z^2)\overrightarrow {k}.
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(1)

Compute ∇×F→\nabla \times \overrightarrow {F} (the curl of F→\overrightarrow {F}).

(2)

Compute the integral of ∇×F→\nabla \times \overrightarrow {F} over the surface x2+y2+z2=16x^2+y^2+z^2=16, z≥0z \geq 0.

Problem 2.3.8

Let the vector field FF in R3\mathbb {R}^{3} have the form

F(r)=g(∥r∥)r(r≠(0,0,0)), F(r) = g(\left\| r\right\| ) r \qquad (r \neq (0,0,0)),

where gg is a real valued smooth function on (0,∞)(0,\infty ) and ∥⋅∥\left\| \cdot \right\| denotes the Euclidean norm. (FF is undefined at (0,0,0)(0,0,0).) Prove that

∫CF⋅ds=0 \int _C F \cdot ds = 0

for any smooth closed path CC in R3\mathbb {R}^{3} that does not pass through the origin.

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Problem 2.3.9

Let B\mathcal{B} denote the unit ball of R3\mathbb {R}^{3}, B={r∈R3∣∥r∥≤1}\mathcal{B} = \left\{ r \in \mathbb {R}^{3} \mid \left\| r\right\| \leq 1\right\}. Let J→=(J1,J2,J3)\overrightarrow {J} = (J_1, J_2, J_3) be a smooth vector field on R3\mathbb {R}^{3} that vanishes outside of B\mathcal{B} and satisfies ∇⋅J→=0\nabla \cdot \overrightarrow {J} = 0.

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(1)

For ff a smooth, scalar-valued function defined on a neighborhood of B\mathcal{B}, prove that

∫B(∇f)⋅J→ dx dy dz=0. \int _{\mathcal{B}} (\nabla f) \cdot \overrightarrow {J} \, dx \, dy \, dz = 0.
(2)

Prove that

∫BJ1 dx dy dz=0. \int _{\mathcal{B}} J_1 \, dx \, dy \, dz = 0.
Problem 2.3.10

Let D\mathcal{D} denote the open unit disc in R2\mathbb {R}^{2}. Let uu be an eigenfunction for the Laplacian in D\mathcal{D}; that is, a real valued function of class C2C^2 defined in D‾\overline{\mathcal{D}}, zero on the boundary of D\mathcal{D} but not identically zero, and satisfying the differential equation

∂2u∂x2+∂2u∂y2=λu, \frac{\partial ^2 u}{\partial x^2} + \frac{\partial ^2 u}{\partial y^2} = \lambda u,

where λ\lambda is a constant. Prove that

∬D∣grad⁡u∣2 dx dy+λ∬Du2 dx dy=0,(∗) \iint _{\mathcal{D}} \left|\operatorname {grad} u\right|^2 \, dx \, dy + \lambda \iint _{\mathcal{D}} u^2 \, dx \, dy = 0, \tag {$*$}

and hence that λ<0\lambda < 0.

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Problem 2.3.11

Let λ,a∈R\lambda , a \in \mathbb {R}, with a<0a < 0. Let u(x,y)u(x,y) be an infinitely differentiable function defined on an open neighborhood of closed unit disc D\mathcal{D} such that

∂2u∂x2+∂2u∂y2=λuin int⁡(D) \frac{\partial ^2 u}{\partial x^2} + \frac{\partial ^2 u}{\partial y^2} = \lambda u \qquad \text{in } \operatorname {int}(\mathcal{D}) Dnu=auin ∂D. D_n u = au \qquad \text{in } \partial \mathcal{D}.

Here DnuD_n u denotes the directional derivative of uu in the direction of the outward unit normal. Prove that if uu is not identically zero in the interior of D\mathcal{D} then λ<0\lambda < 0.

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Problem 2.3.12

Let ff be a one-to-one C1C^1 map of R3\mathbb {R}^{3} into R3\mathbb {R}^{3}, and let JJ denote its Jacobian determinant. Prove that if x0x_0 is any point of R3\mathbb {R}^{3} and Qr(x0)Q_r(x_0) denotes the cube with center x0x_0, side length rr, and edges parallel to the coordinate axes, then

∣J(x0)∣=lim⁡r→0r−3vol⁡(f(Qr(x0)))≤lim sup⁡x→x0∥f(x)−f(x0)∥3∥x−x0∥3. \left|J(x_0)\right| = \lim _{r \to 0} r^{-3} \operatorname {vol}(f(Q_r(x_0))) \leq \limsup _{x \to x_0} \frac{\left\| f(x)-f(x_0)\right\| ^3}{\left\| x-x_0\right\| ^3}.

Here, ∥⋅∥\left\| \cdot \right\| is the Euclidean norm in R3\mathbb {R}^{3}.

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