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Multiple Integrals

3.2 Double Integrals in Polar Coordinates

24 problems · hints, answers and solutions shown beside each one

1Stage 1Conceptual

Do you understand the idea? Usually little or no calculation.

Q1Stage 1

Consider the points

(x1,y1)=(3,0)(x2,y2)=(1,1)(x3,y3)=(0,1)(x4,y4)=(1,1)(x5,y5)=(2,0)\begin{align*} (x_1,y_1) &= (3,0) & (x_2,y_2) &= (1,1) & (x_3,y_3) &= (0,1) \\ (x_4,y_4) &= (-1,1) & (x_5,y_5) &= (-2,0) \end{align*}

For each 1i51\le i\le 5,

  • sketch, in the xyxy-plane, the point (xi,yi)(x_i,y_i) and

  • find polar coordinates rir_i and θi\theta_i, with ri>0r_i>0 and 0θi<2π0\le\theta_i<2\pi, for the point (xi,yi)(x_i,y_i).

Answer

The left hand sketch below contains the points, (x1,y1)(x_1,y_1), (x3,y3)(x_3,y_3), (x5,y5)(x_5,y_5), that are on the axes. The right hand sketch below contains the points, (x2,y2)(x_2,y_2), (x4,y4)(x_4,y_4), that are not on the axes.

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

r1=3r_1 = 3, θ1=0\theta_1=0 r2=2r_2 = \sqrt{2}, θ2=π4\theta_2=\frac{\pi}{4} r3=1r_3 = 1, θ3=π2\theta_3=\frac{\pi}{2} r4=2r_4 = \sqrt{2}, θ4=3π4\theta_4=\frac{3\pi}{4}
r5=2r_5 = 2, θ5=π\theta_5=\pi

Full solution

The left hand sketch below contains the points, (x1,y1)(x_1,y_1), (x3,y3)(x_3,y_3), (x5,y5)(x_5,y_5), that are on the axes. The right hand sketch below contains the points, (x2,y2)(x_2,y_2), (x4,y4)(x_4,y_4), that are not on the axes.

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

Figure from prob_s3.2, line 39

Recall that the polar coordinates rr, θ\theta are related to the cartesian coordinates xx, yy, by x=rcosθx=r\cos\theta, y=rsinθy=r\sin\theta. So r=x2+y2r=\sqrt{x^2+y^2} and tanθ=yx\tan\theta=\frac{y}{x} (assuming that x0x\ne 0 and r>0r>0) and

(x1,y1)=(3,0)    r1=3, tanθ1=0    θ1=0 as (x1,y1) is on the positive x-axis(x2,y2)=(1,1)    r2=2, tanθ2=1    θ2=π4 as (x2,y2) is in the first octant(x3,y3)=(0,1)    r3=1, cosθ3=0    θ3=π2 as (x3,y3) is on the positive y-axis(x4,y4)=(1,1)    r4=2, tanθ4=1    θ4=3π4 as (x4,y4) is in the third octant(x5,y5)=(2,0)    r5=2, tanθ5=0    θ5=π as (x5,y5) is on the negative x-axis\begin{alignat*}{5} (x_1,y_1) &= (3,0) &&\implies &r_1=3,\ \tan\theta_1=0 &&\implies \theta_1&=0 \text{ as }(x_1,y_1)\text{ is on the positive }x\text{-axis} \\ (x_2,y_2) &= (1,1) &&\implies &r_2=\sqrt{2},\ \tan\theta_2=1 &&\implies \theta_2&=\frac{\pi}{4} \text{ as }(x_2,y_2)\text{ is in the first octant} \\ (x_3,y_3) &= (0,1) &&\implies &r_3=1,\ \cos\theta_3=0 &&\implies \theta_3&=\frac{\pi}{2} \text{ as }(x_3,y_3)\text{ is on the positive }y\text{-axis} \\ (x_4,y_4) &= (-1,1) &&\implies &r_4=\sqrt{2},\ \tan\theta_4=-1 &&\implies \theta_4&=\frac{3\pi}{4} \text{ as }(x_4,y_4)\text{ is in the third octant} \\ (x_5,y_5) &= (-2,0) &&\implies &r_5=2,\ \tan\theta_5=0 &&\implies \theta_5&=\pi \text{ as }(x_5,y_5)\text{ is on the negative }x\text{-axis} \end{alignat*}
Q2Stage 1

For each of the following points (xi,yi)(x_i,y_i),

  • find all pairs (ri,θi)(r_i,\theta_i) such that (xi,yi)=(ricosθi,risinθi)(x_i,y_i) = \big(r_i\cos\theta_i\,,\,r_i\sin\theta_i\big), and

  • in particular, find a pair (ri,θi)(r_i,\theta_i) with ri<0r_i<0 and 0θi<2π0\le\theta_i<2\pi such that (xi,yi)=(ricosθi,risinθi)(x_i,y_i) = \big(r_i\cos\theta_i\,,\,r_i\sin\theta_i\big)

  1. (x1,y1)=(2,0)(x_1,y_1) = (-2,0)

  2. (x2,y2)=(1,1)(x_2,y_2) = (1,1)

  3. (x3,y3)=(1,1)(x_3,y_3) = (-1,-1)

  4. (x4,y4)=(3,0)(x_4,y_4) = (3,0)

  5. (x5,y5)=(0,1)(x_5,y_5) = (0,1)

Hint

rr is allowed to be negative.

Answer

(a) (r1=2,θ1=nπ, n odd integer )\big(r_1=2\,,\,\theta_1= n\pi,\ n\text{ odd integer }\big) or (r1=2,θ1=nπ, n even integer )\big(r_1=-2\,,\,\theta_1= n\pi,\ n\text{ even integer }\big). In particular, (r1=2,θ1=0)\big(r_1=-2\,,\,\theta_1= 0\big) has r1<0r_1<0 and 0θ1<2π0\le\theta_1<2\pi.

(b) (r2=2,θ2=π ⁣/4+2nπ)\big(r_2=\sqrt{2}\,,\,\theta_2= \nicefrac{\pi}{4} + 2n\pi\big) or (r2=2,θ2=5π ⁣/4+2nπ)\big(r_2=-\sqrt{2}\,,\,\theta_2= \nicefrac{5\pi}{4} + 2n\pi\big), with nn integer. In particular, (r2=2,θ2=5π ⁣/4)\big(r_2=-\sqrt{2}\,,\, \theta_2= \nicefrac{5\pi}{4}\big) has r2<0r_2<0 and 0θ2<2π0\le\theta_2<2\pi.

(c) (r3=2,θ3=5π ⁣/4+2nπ)\big(r_3=\sqrt{2}\,,\,\theta_3= \nicefrac{5\pi}{4} + 2n\pi\big) or (r3=2,θ3=π ⁣/4+2nπ)\big(r_3=-\sqrt{2}\,,\,\theta_3= \nicefrac{\pi}{4} + 2n\pi\big), with nn integer. In particular, (r3=2,θ3=π ⁣/4)\big(r_3=-\sqrt{2}\,,\, \theta_3= \nicefrac{\pi}{4}\big) has r3<0r_3<0 and 0θ3<2π0\le\theta_3<2\pi.

(d) (r4=3,θ4=0+2nπ)\big(r_4=3\,,\,\theta_4= 0 + 2n\pi\big) or (r4=3,θ4=π+2nπ)\big(r_4=-3\,,\,\theta_4= \pi + 2n\pi\big), with nn integer. In particular, (r4=3,θ4=π)\big(r_4=-3\,,\, \theta_4= \pi\big) has r4<0r_4<0 and 0θ4<2π0\le\theta_4<2\pi.

(e) (r5=1,θ5=π ⁣/2+2nπ)\big(r_5=1\,,\,\theta_5= \nicefrac{\pi}{2} + 2n\pi\big) or (r5=1,θ5=3π ⁣/2+2nπ)\big(r_5=-1\,,\,\theta_5= \nicefrac{3\pi}{2} + 2n\pi\big), with nn integer. In particular, (r5=1,θ5=3π ⁣/2)\big(r_5=-1\,,\, \theta_5= \nicefrac{3\pi}{2}\big) has r5<0r_5<0 and 0θ5<2π0\le\theta_5<2\pi.

Full solution

In this solution, we'll supress the subscripts. That is, we'll write rr in place of rir_i and θ\theta in place of θi\theta_i. Note that the distance from the point (rcosθ,rsinθ)\big(r\cos\theta\,,\,r\sin\theta\big) to the origin is

r2cos2θ+r2sin2θ=r2=r\begin{equation*} \sqrt{r^2\cos^2\theta + r^2\sin^2\theta} =\sqrt{r^2} =|r| \end{equation*}

Thus rr can be either the distance to the origin or minus the distance to the origin.

(a) The distance from (2,0)(-2,0) to the origin is 22. So either r=2r=2 or r=2r=-2.

  • If r=2r=2, then θ\theta must obey

    (2,0)=(2cosθ,2sinθ)    sinθ=0, cosθ=1    θ=nπ, n integer , cosθ=1    θ=nπ, n odd integer \begin{align*} (-2,0) = \big(2\cos\theta\,,\,2\sin\theta\big) &\iff \sin\theta=0,\ \cos\theta=-1 \\ &\iff \theta= n\pi,\ n\text{ integer },\ \cos\theta=-1 \\ &\iff \theta= n\pi,\ n\text{ odd integer } \end{align*}
  • If r=2r=-2, then θ\theta must obey

    (2,0)=(2cosθ,2sinθ)    sinθ=0, cosθ=1    θ=nπ, n integer , cosθ=1    θ=nπ, n even integer \begin{align*} (-2,0) = \big(-2\cos\theta\,,\,-2\sin\theta\big) &\iff \sin\theta=0,\ \cos\theta=1 \\ &\iff \theta= n\pi,\ n\text{ integer },\ \cos\theta=1 \\ &\iff \theta= n\pi,\ n\text{ even integer } \end{align*}

In particular, (r=2,θ=0)\big(r=-2\,,\,\theta= 0\big) has r<0r<0 and 0θ<2π0\le\theta<2\pi.

In the figure on the left below, the blue half-line is the set of all points with polar coordinates θ=π\theta=\pi, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=π\theta=\pi, r<0r<0. In the figure on the right below, the blue half-line is the set of all points with polar coordinates θ=0\theta=0, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=0\theta=0, r<0r<0.

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

(b) The distance from (1,1)(1,1) to the origin is 2\sqrt{2}. So either r=2r=\sqrt{2} or r=2r=-\sqrt{2}.

  • If r=2r=\sqrt{2}, then θ\theta must obey

    (1,1)=(2cosθ,2sinθ)    sinθ=cosθ=1 ⁣/2    θ=π ⁣/4+2nπ, n integer \begin{align*} (1,1) = \big(\sqrt{2}\,\cos\theta\,,\,\sqrt{2}\,\sin\theta\big) &\iff \sin\theta=\cos\theta=\nicefrac{1}{\sqrt{2}} \\ &\iff \theta= \nicefrac{\pi}{4} + 2n\pi,\ n\text{ integer } \end{align*}
  • If r=2r=-\sqrt{2}, then θ\theta must obey

    (1,1)=(2cosθ,2sinθ)    sinθ=cosθ=1 ⁣/2    θ=5π ⁣/4+2nπ, n integer \begin{align*} (1,1) = \big(-\sqrt{2}\,\cos\theta\,,\,-\sqrt{2}\,\sin\theta\big) &\iff \sin\theta=\cos\theta=-\nicefrac{1}{\sqrt{2}} \\ &\iff \theta= \nicefrac{5\pi}{4} + 2n\pi,\ n\text{ integer } \end{align*}

In particular, (r=2,θ=5π ⁣/4)\big(r=-\sqrt{2}\,,\, \theta= \nicefrac{5\pi}{4}\big) has r<0r<0 and 0θ<2π0\le\theta<2\pi.

In the figure on the left below, the blue half-line is the set of all points with polar coordinates θ=π4\theta=\frac{\pi}{4}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=π4\theta=\frac{\pi}{4}, r<0r<0. In the figure on the right below, the blue half-line is the set of all points with polar coordinates θ=5π4\theta=\frac{5\pi}{4}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=5π4\theta=\frac{5\pi}{4}, r<0r<0.

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

(c) The distance from (1,1)(-1,-1) to the origin is 2\sqrt{2}. So either r=2r=\sqrt{2} or r=2r=-\sqrt{2}.

  • If r=2r=\sqrt{2}, then θ\theta must obey

    (1,1)=(2cosθ,2sinθ)    sinθ=cosθ=1 ⁣/2    θ=5π ⁣/4+2nπ, n integer \begin{align*} (-1,-1) = \big(\sqrt{2}\,\cos\theta\,,\,\sqrt{2}\,\sin\theta\big) &\iff \sin\theta=\cos\theta=-\nicefrac{1}{\sqrt{2}} \\ &\iff \theta= \nicefrac{5\pi}{4} + 2n\pi,\ n\text{ integer } \end{align*}
  • If r=2r=-\sqrt{2}, then θ\theta must obey

    (1,1)=(2cosθ,2sinθ)    sinθ=cosθ=1 ⁣/2    θ=π ⁣/4+2nπ, n integer \begin{align*} (-1,-1) = \big(-\sqrt{2}\,\cos\theta\,,\,-\sqrt{2}\,\sin\theta\big) &\iff \sin\theta=\cos\theta=\nicefrac{1}{\sqrt{2}} \\ &\iff \theta= \nicefrac{\pi}{4} + 2n\pi,\ n\text{ integer } \end{align*}

In particular, (r=2,θ=π ⁣/4)\big(r=-\sqrt{2}\,,\, \theta= \nicefrac{\pi}{4}\big) has r<0r<0 and 0θ<2π0\le\theta<2\pi.

In the figure on the left below, the blue half-line is the set of all points with polar coordinates θ=5π4\theta=\frac{5\pi}{4}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=5π4\theta=\frac{5\pi}{4}, r<0r<0. In the figure on the right below, the blue half-line is the set of all points with polar coordinates θ=π4\theta=\frac{\pi}{4}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=π4\theta=\frac{\pi}{4}, r<0r<0.

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

(d) The distance from (3,0)(3,0) to the origin is 33. So either r=3r=3 or r=3r=-3.

  • If r=3r=3, then θ\theta must obey

    (3,0)=(3cosθ,3sinθ)    sinθ=0, cosθ=1    θ=0+2nπ, n integer \begin{align*} (3,0) = \big(3\,\cos\theta\,,\,3\,\sin\theta\big) &\iff \sin\theta=0,\ \cos\theta=1 \\ &\iff \theta= 0 + 2n\pi,\ n\text{ integer } \end{align*}
  • If r=3r=-3, then θ\theta must obey

    (3,0)=(3cosθ,3sinθ)    sinθ=0, cosθ=1    θ=π+2nπ, n integer \begin{align*} (3,0) = \big(-3\,\cos\theta\,,\,-3\,\sin\theta\big) &\iff \sin\theta=0,\ \cos\theta=-1 \\ &\iff \theta= \pi + 2n\pi,\ n\text{ integer } \end{align*}

In particular, (r=3,θ=π)\big(r=-3\,,\, \theta= \pi\big) has r<0r<0 and 0θ<2π0\le\theta<2\pi.

In the figure on the left below, the blue half-line is the set of all points with polar coordinates θ=π\theta=\pi, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=π\theta=\pi, r<0r<0. In the figure on the right below, the blue half-line is the set of all points with polar coordinates θ=0\theta=0, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=0\theta=0, r<0r<0.

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

(e) The distance from (0,1)(0,1) to the origin is 11. So either r=1r=1 or r=1r=-1.

  • If r=1r=1, then θ\theta must obey

    (0,1)=(cosθ,sinθ)    cosθ=0, sinθ=1    θ=π ⁣/2+2nπ, n integer \begin{align*} (0,1) = \big(\cos\theta\,,\,\sin\theta\big) &\iff \cos\theta=0,\ \sin\theta=1 \\ &\iff \theta= \nicefrac{\pi}{2} + 2n\pi,\ n\text{ integer } \end{align*}
  • If r=1r=-1, then θ\theta must obey

    (0,1)=(cosθ,sinθ)    cosθ=0, sinθ=1    θ=3π ⁣/2+2nπ, n integer \begin{align*} (0,1) = \big(-\cos\theta\,,\,-\sin\theta\big) &\iff \cos\theta=0,\ \sin\theta=-1 \\ &\iff \theta= \nicefrac{3\pi}{2} + 2n\pi,\ n\text{ integer } \end{align*}

In particular, (r=1,θ=3π ⁣/2)\big(r=-1\,,\, \theta= \nicefrac{3\pi}{2}\big) has r<0r<0 and 0θ<2π0\le\theta<2\pi.

In the figure on the left below, the blue half-line is the set of all points with polar coordinates θ=3π2\theta=\frac{3\pi}{2}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=3π2\theta=\frac{3\pi}{2}, r<0r<0. In the figure on the right below, the blue half-line is the set of all points with polar coordinates θ=π2\theta=\frac{\pi}{2}, r>0r>0 and the orange half-line is the set of all points with polar coordinates θ=π2\theta=\frac{\pi}{2}, r<0r<0.

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Figure from prob_s3.2, line 149

Q3Stage 1

Consider the points

(x1,y1)=(3,0)(x2,y2)=(1,1)(x3,y3)=(0,1)(x4,y4)=(1,1)(x5,y5)=(2,0)\begin{align*} (x_1,y_1) &= (3,0) & (x_2,y_2) &= (1,1) & (x_3,y_3) &= (0,1) \\ (x_4,y_4) &= (-1,1) & (x_5,y_5) &= (-2,0) \end{align*}

Also define, for each angle θ\theta, the vectors

e^r(θ)=cosθ ı^+sinθ ȷ^e^θ(θ)=sinθ ı^+cosθ ȷ^\begin{align*} \he_r(\theta)=\cos\theta\ \hi + \sin\theta\ \hj\qquad \he_\theta(\theta) = -\sin\theta\ \hi + \cos\theta\ \hj \end{align*}
  1. Determine, for each angle θ\theta, the lengths of the vectors e^r(θ)\he_r(\theta) and e^θ(θ)\he_\theta(\theta) and the angle between the vectors e^r(θ)\he_r(\theta) and e^θ(θ)\he_\theta(\theta). Compute e^r(θ)×e^θ(θ)\he_r(\theta)\times\he_\theta(\theta) (viewing e^r(θ)\he_r(\theta) and e^θ(θ)\he_\theta(\theta) as vectors in three dimensions with zero k^\hk components).

  2. For each 1i51\le i\le 5, sketch, in the xyxy-plane, the point (xi,yi)=(ricosθi,risinθi)(x_i,y_i)= \big(r_i\cos\theta_i\,,\,r_i\sin\theta_i\big) and the vectors e^r(θi)\he_r(\theta_i) and e^θ(θi)\he_\theta(\theta_i). In your sketch of the vectors, place the tails of the vectors e^r(θi)\he_r(\theta_i) and e^θ(θi)\he_\theta(\theta_i) at (xi,yi)(x_i,y_i).

Hint

Compute, for each angle θ\theta, the dot product e^r(θ)e^θ(θ)\he_r(\theta)\cdot\he_\theta(\theta).

Answer

(a) Both e^r(θ)\he_r(\theta) and e^θ(θ)\he_\theta(\theta) have length 1. The angle between them is π2\frac{\pi}{2}. The cross product is e^r(θ)×e^θ(θ)=k^\he_r(\theta) \times \he_\theta(\theta)=\hk.

(b) Here is a sketch of (xi,yi)(x_i,y_i), e^r(θi)\he_r(\theta_i), e^θ(θi)\he_\theta(\theta_i) for i=1,3,5i =1,3,5 (the points on the axes)

Figure from prob_s3.2, line 365

Figure from prob_s3.2, line 365

and here is a sketch (to a different scale) of (xi,yi)(x_i,y_i), e^r(θi)\he_r(\theta_i), e^θ(θi)\he_\theta(\theta_i) for i=2,4i =2,4 (the points off the axes).

Figure from prob_s3.2, line 365

Figure from prob_s3.2, line 365

Full solution

(a) The lengths are

e^r(θ)=cos2θ+sin2θ=1e^θ(θ)=(sinθ)2+cos2θ=1\begin{align*} |\he_r(\theta)| &= \sqrt{\cos^2\theta+\sin^2\theta} = 1 \\ |\he_\theta(\theta)| &= \sqrt{(-\sin\theta)^2+\cos^2\theta} = 1 \end{align*}

As

e^r(θ)e^θ(θ)=(cosθ)(sinθ)+(sinθ)(cosθ)=0\begin{equation*} \he_r(\theta) \cdot \he_\theta(\theta) = (\cos\theta)(-\sin\theta) +(\sin\theta)(\cos\theta)=0 \end{equation*}

the two vectors are perpendicular and the angle between them is π2\frac{\pi}{2}. The cross product is

e^r(θ)×e^θ(θ)=det[ı^ȷ^k^cosθsinθ0sinθcosθ0]=k^\begin{align*} \he_r(\theta) \times \he_\theta(\theta) &=\det\left[\begin{matrix} \hi & \hj & \hk \\ \cos\theta & \sin\theta & 0 \\ -\sin\theta & \cos\theta & 0 \end{matrix}\right] =\hk \end{align*}

(b) Note that for θ\theta determined by x=rcosθx=r\cos\theta, y=rsinθy=r\sin\theta,

  • the vector e^r(θ)\he_r(\theta) is a unit vector in the same direction as the vector from (0,0)(0,0) to (x,y)(x,y) and

  • the vector e^θ(θ)\he_\theta(\theta) is a unit vector that is perpendicular to e^r(θ)\he_r(\theta).

  • The yy-component of e^θ(θ)\he_\theta(\theta) has the same sign as the xx-component of e^r(θ)\he_r(\theta). The xx-component of e^θ(θ)\he_\theta(\theta) has opposite sign to that of the yy-component of e^r(θ)\he_r(\theta).

Here is a sketch of (xi,yi)(x_i,y_i), e^r(θi)\he_r(\theta_i), e^θ(θi)\he_\theta(\theta_i) for i=1,3,5i =1,3,5 (the points on the axes)

Figure from prob_s3.2, line 365

Figure from prob_s3.2, line 365

and here is a sketch (to a different scale) of (xi,yi)(x_i,y_i), e^r(θi)\he_r(\theta_i), e^θ(θi)\he_\theta(\theta_i) for i=2,4i =2,4 (the points off the axes).

Figure from prob_s3.2, line 365

Figure from prob_s3.2, line 365

Q4Stage 1

Let <a,b>\llt a, b\rgt be a vector. Let rr be the length of <a,b>\llt a, b\rgt and θ\theta be the angle between <a,b>\llt a, b\rgt and the xx-axis.

  1. Express aa and bb in terms of rr and θ\theta.

  2. Let <A,B>\llt A, B\rgt be the vector gotten by rotating <a,b>\llt a, b\rgt by an angle φ\varphi about its tail. Express AA and BB in terms of aa, bb and φ\varphi.

Hint

Sketch <a,b>\llt a, b\rgt and <A,B>\llt A, B\rgt. The trigonometric addition formulas

sin(θ+φ)=sinθcosφ+cosθsinφcos(θ+φ)=cosθcosφsinθsinφ\begin{align*} \sin(\theta+\varphi) &=\sin\theta\cos\varphi+\cos\theta\sin\varphi \\ \cos(\theta+\varphi) &=\cos\theta\cos\varphi-\sin\theta\sin\varphi \end{align*}

will help.

Answer

(a) a=rcosθa=r\cos\theta, b=rsinθb=r\sin\theta

(b) A=acosφbsinφA=a\cos\varphi-b\sin\varphi, B=bcosφ+asinφB=b\cos\varphi+a\sin\varphi

Full solution

Here is a sketch of <a,b>\llt a, b\rgt and <A,B>\llt A, B\rgt.

Figure from prob_s3.2, line 464

Figure from prob_s3.2, line 464

(a) From the sketch,

a=rcosθb=rsinθ\begin{align*} a&=r\cos\theta\\ b&=r\sin\theta \end{align*}

(b) The length of the vector <A,B>\llt A, B\rgt is again rr and the angle between <A,B>\llt A, B\rgt and the xx-axis is θ+φ\theta +\varphi. So

A=rcos(θ+φ)=rcosθcosφrsinθsinφ=acosφbsinφB=rsin(θ+φ)=rsinθcosφ+rcosθsinφ=bcosφ+asinφ\begin{alignat*}{3} A&=r\cos(\theta+\varphi) &&=r\cos\theta\cos\varphi-r\sin\theta\sin\varphi &&=a\cos\varphi-b\sin\varphi\\ B&=r\sin(\theta+\varphi) &&=r\sin\theta\cos\varphi+r\cos\theta\sin\varphi &&=b\cos\varphi+a\sin\varphi \end{alignat*}
Q5Stage 1

For each of the regions R\cR sketched below, express Rf(x,y)dxdy\dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} as an iterated integral in polar coordinates in two different ways.

(a)

Figure from prob_s3.2, line 490

Figure from prob_s3.2, line 490

(b)

Figure from prob_s3.2, line 490

Figure from prob_s3.2, line 490

(c)

Figure from prob_s3.2, line 490

Figure from prob_s3.2, line 490

(d)

Figure from prob_s3.2, line 490

Figure from prob_s3.2, line 490

Answer

(a) Rf(x,y)dxdy=0π ⁣/4dθ02dr r f(rcosθ,rsinθ)=02dr0π ⁣/4dθ r f(rcosθ,rsinθ)\displaystyle\dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{4}}\dee{\theta} \int_0^2\dee{r}\ r\ f(r\cos\theta,r\sin\theta) =\int_0^2\dee{r} \int_0^{\nicefrac{\pi}{4}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta)

(b) Rf(x,y)dxdy=0π ⁣/2dθ12dr r f(rcosθ,rsinθ)=12dr0π ⁣/2dθ r f(rcosθ,rsinθ)\displaystyle\dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{2}}\dee{\theta} \int_1^2\dee{r}\ r\ f(r\cos\theta,r\sin\theta) =\int_1^2\dee{r} \int_0^{\nicefrac{\pi}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta)

(c) Rf(x,y)dxdy=0π ⁣/2dθ02cosθdr r f(rcosθ,rsinθ)=02dr0arccosr2dθ r f(rcosθ,rsinθ)\displaystyle \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{2}}\dee{\theta} \int_0^{2\cos\theta}\dee{r}\ r\ f(r\cos\theta,r\sin\theta) =\int_0^2\dee{r} \int_0^{\arccos\frac{r}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta)

(d)

Rf(x,y)dxdy=π ⁣/4π ⁣/2dθ02 ⁣/sinθdr r f(rcosθ,rsinθ)=02drπ ⁣/4π ⁣/2dθ r f(rcosθ,rsinθ)+222drπ ⁣/4arcsin2rdθ r f(rcosθ,rsinθ)\begin{align*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} &=\int_{\nicefrac{\pi}{4}}^{\nicefrac{\pi}{2}}\dee{\theta} \int_0^{\nicefrac{2}{\sin\theta}}\dee{r}\ r\ f(r\cos\theta,r\sin\theta)\\ &=\int_0^2\dee{r} \int_{\nicefrac{\pi}{4}}^{\nicefrac{\pi}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) +\int_2^{2\sqrt{2}}\dee{r} \int_{\nicefrac{\pi}{4}}^{\arcsin\frac{2}{r}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) \end{align*}
Full solution

(a) The region

R={ (x,y)  0x2+y24, 0yx }\begin{equation*} \cR=\Set{(x,y)}{0\le x^2+y^2\le 4,\ 0\le y\le x} \end{equation*}

In polar coordinates,

  • the circle x2+y2=4x^2+y^2=4 becomes r2=4r^2=4 or r=2r=2 and

  • the line y=xy=x becomes rsinθ=rcosθr\sin\theta=r\cos\theta or tanθ=1\tan\theta=1 or θ=π4\theta=\frac{\pi}{4}.

Thus the domain of integration is

R={ (rcosθ,rsinθ)  0r2, 0θπ4 }\begin{equation*} \cR=\Set{(r\cos\theta,r\sin\theta)}{0\le r\le 2,\ 0\le\theta\le\tfrac{\pi}{4}} \end{equation*}

On this domain,

  • θ\theta runs from 00 to π4\frac{\pi}{4}.

  • For each fixed θ\theta in that range, rr runs from 00 to 22, as in the figure on the left below.

In polar coordinates dxdy=rdrdθ\dee{x}\,\dee{y} = r\,\dee{r}\,\dee{\theta}, so that

Rf(x,y)dxdy=0π ⁣/4dθ02dr r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{4}}\dee{\theta} \int_0^2\dee{r}\ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Alternatively, on R\cR,

  • rr runs from 00 to 22.

  • For each fixed rr in that range, θ\theta runs from 00 to π4\frac{\pi}{4}, as in the figure on the right above.

So

Rf(x,y)dxdy=02dr0π ⁣/4dθ r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^2\dee{r} \int_0^{\nicefrac{\pi}{4}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

(b) The region

R={ (x,y)  1x2+y24, x0, y0 }\begin{equation*} \cR=\Set{(x,y)}{1\le x^2+y^2\le 4,\ x\ge 0,\ y\ge 0} \end{equation*}

In polar coordinates,

  • the circle x2+y2=1x^2+y^2=1 becomes r2=1r^2=1 or r=1r=1 and

  • the circle x2+y2=4x^2+y^2=4 becomes r2=4r^2=4 or r=2r=2 and

  • the positive xx-axis, x0x\ge0, y=0y=0, becomes θ=0\theta=0 and

  • the positive yy-axis, x=0x=0, y0y\ge0, becomes θ=π2\theta=\frac{\pi}{2}.

Thus the domain of integration is

R={ (rcosθ,rsinθ)  1r2, 0θπ2 }\begin{equation*} \cR=\Set{(r\cos\theta,r\sin\theta)}{1\le r\le 2,\ 0\le\theta\le\tfrac{\pi}{2}} \end{equation*}

On this domain,

  • θ\theta runs from 00 to π2\frac{\pi}{2}.

  • For each fixed θ\theta in that range, rr runs from 11 to 22, as in the figure on the left below.

In polar coordinates dxdy=rdrdθ\dee{x}\,\dee{y} = r\,\dee{r}\,\dee{\theta}, so that

Rf(x,y)dxdy=0π ⁣/2dθ12dr r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{2}}\dee{\theta} \int_1^2\dee{r}\ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Alternatively, on R\cR,

  • rr runs from 11 to 22.

  • For each fixed rr in that range, θ\theta runs from 00 to π2\frac{\pi}{2}, as in the figure on the right above.

So

Rf(x,y)dxdy=12dr0π ⁣/2dθ r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_1^2\dee{r} \int_0^{\nicefrac{\pi}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

(c) The region

R={ (x,y)  (x1)2+y21, y0 }\begin{equation*} \cR=\Set{(x,y)}{(x-1)^2+y^2\le 1,\ y \ge 0} \end{equation*}

In polar coordinates, the circle (x1)2+y2=1(x-1)^2+y^2= 1, or x22x+y2=0x^2-2x+y^2=0, is r22rcosθ=0r^2-2r\cos\theta=0 or r=2cosθr=2\cos\theta. Note that, on r=2cosθr=2\cos\theta,

  • when θ=0\theta=0, r=2r=2 and

  • as θ\theta increases from 00 towards π ⁣/2\nicefrac{\pi}{2}, rr decreases but remains strictly bigger than 00 (look at the figure below), until

  • when θ=π2\theta=\frac{\pi}{2}, r=0r=0.

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Thus the domain of integration is

R={ (rcosθ,rsinθ)  0θπ2, 0r2cosθ }\begin{equation*} \cR=\Set{(r\cos\theta,r\sin\theta)}{0\le\theta\le\tfrac{\pi}{2},\ 0\le r\le 2\cos\theta} \end{equation*}

On this domain,

  • θ\theta runs from 00 to π2\frac{\pi}{2}.

  • For each fixed θ\theta in that range, rr runs from 00 to 2cosθ2\cos\theta, as in the figure on the left below.

In polar coordinates dxdy=rdrdθ\dee{x}\,\dee{y} = r\,\dee{r}\,\dee{\theta}, so that

Rf(x,y)dxdy=0π ⁣/2dθ02cosθdr r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^{\nicefrac{\pi}{2}}\dee{\theta} \int_0^{2\cos\theta}\dee{r}\ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Alternatively, on R\cR,

  • rr runs from 00 (at the point (0,0)(0,0))
    to 22 (at the point (2,0)(2,0)).

  • For each fixed rr in that range, θ\theta runs from 00 to arccosr2\arccos\frac{r}{2} (which was gotten by solving r=2cosθr=2\cos\theta for θ\theta as a function of rr), as in the figure on the right above.

So

Rf(x,y)dxdy=02dr0arccosr2dθ r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^2\dee{r} \int_0^{\arccos\frac{r}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

(d) The region

R={ (x,y)  0y2, 0xy }\begin{equation*} \cR=\Set{(x,y)}{0\le y\le 2,\ 0\le x\le y} \end{equation*}

In polar coordinates,

  • the line y=2y=2 becomes rsinθ=2r\sin\theta=2 and

  • the positive yy-axis, x=0x=0, y0y\ge0, becomes θ=π2\theta=\frac{\pi}{2} and

  • the line y=xy=x becomes rsinθ=rcosθr\sin\theta=r\cos\theta or tanθ=1\tan\theta=1 or θ=π4\theta=\frac{\pi}{4}.

Thus the domain of integration is

R={ (rcosθ,rsinθ)  π4θπ2, 0rsinθ2 }\begin{equation*} \cR=\Set{(r\cos\theta,r\sin\theta)}{\tfrac{\pi}{4}\le\theta\le\tfrac{\pi}{2},\ 0\le r\sin\theta\le 2} \end{equation*}

On this domain,

  • θ\theta runs from π4\frac{\pi}{4} to π2\frac{\pi}{2}.

  • For each fixed θ\theta in that range, rr runs from 00 to 2sinθ\frac{2}{\sin\theta}, as in the figure on the left below.

In polar coordinates dxdy=rdrdθ\dee{x}\,\dee{y} = r\,\dee{r}\,\dee{\theta}, so that

Rf(x,y)dxdy=π ⁣/4π ⁣/2dθ02 ⁣/sinθdr r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_{\nicefrac{\pi}{4}}^{\nicefrac{\pi}{2}}\dee{\theta} \int_0^{\nicefrac{2}{\sin\theta}}\dee{r}\ r\ f(r\cos\theta,r\sin\theta) \end{equation*}

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Figure from prob_s3.2, line 549

Alternatively, on R\cR,

  • rr runs from 00 (at the point (0,0)(0,0))
    to 222\sqrt{2} (at the point (2,2)(2,2)).

  • For each fixed rr between 00 and 22, θ\theta runs from π4\frac{\pi}{4} to π2\frac{\pi}{2}, as in the central figure above.

  • For each fixed rr between 22 and 222\sqrt{2}, θ\theta runs from π4\frac{\pi}{4} to arcsin2r\arcsin\frac{2}{r} (which was gotten by solving rsinθ=2r\sin\theta=2 for θ\theta as a function of rr), as in the figure on the right above.

So

Rf(x,y)dxdy=02drπ ⁣/4π ⁣/2dθ r f(rcosθ,rsinθ)+222drπ ⁣/4arcsin2rdθ r f(rcosθ,rsinθ)\begin{equation*} \dblInt_\cR f(x,y)\,\dee{x}\,\dee{y} =\int_0^2\dee{r} \int_{\nicefrac{\pi}{4}}^{\nicefrac{\pi}{2}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) +\int_2^{2\sqrt{2}}\dee{r} \int_{\nicefrac{\pi}{4}}^{\arcsin\frac{2}{r}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta) \end{equation*}
Q6Stage 1

Sketch the domain of integration in the xyxy-plane for each of the following polar coordinate integrals.

  1. 12drπ ⁣/4π ⁣/4dθ r f(rcosθ,rsinθ)\displaystyle \int_1^2\dee{r} \int_{-\nicefrac{\pi}{4}}^{\nicefrac{\pi}{4}}\dee{\theta} \ r\ f(r\cos\theta,r\sin\theta)

  2. 0π ⁣/4dθ02sinθ+cosθdr r f(rcosθ,rsinθ)\displaystyle \int_0^{\nicefrac{\pi}{4}}\dee{\theta} \int_0^{\frac{2}{\sin\theta+\cos\theta}}\dee{r} \ r\ f(r\cos\theta,r\sin\theta)

  3. 02πdθ03cos2θ+9sin2θdr r f(rcosθ,rsinθ)\displaystyle \int_0^{2\pi}\dee{\theta} \int_0^{\frac{3}{\sqrt{\cos^2\theta+9\sin^2\theta}}}\dee{r} \ r\ f(r\cos\theta,r\sin\theta)

Answer

(a)

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

(b)

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

(c)

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

Full solution

(a) Let DD denote the domain of integration. The symbols 12drπ ⁣/4π ⁣/4dθ\displaystyle \int_1^2\dee{r} \int_{-\nicefrac{\pi}{4}}^{\nicefrac{\pi}{4}}\dee{\theta} say that, on DD,

  • rr runs from 11 to 22 and

  • for each rr in that range, θ\theta runs from π4-\frac{\pi}{4} to π4\frac{\pi}{4}.

In Cartesian coordinates

  • r=1r=1 is the circle x2+y2=1x^2+y^2=1 and

  • r=2r=2 is the circle x2+y2=4x^2+y^2=4 and

  • θ=π4\theta=\frac{\pi}{4} is the ray y=xy=x, x0x\ge 0 and

  • θ=π4\theta=-\frac{\pi}{4} is the ray y=xy=-x, x0x\ge 0.

So

D={ (x,y)  1x2+y24, xyx, x0 }\begin{align*} D=\Set{(x,y)}{1\le x^2+y^2\le 4,\ -x\le y\le x,\ x\ge 0} \end{align*}

Here are two sketches. DD is the shaded region in the sketch on the right.

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

(b) Let DD denote the domain of integration. The symbols 0π ⁣/4dθ02sinθ+cosθdr\int_0^{\nicefrac{\pi}{4}}\dee{\theta} \int_0^{\frac{2}{\sin\theta+\cos\theta}}\dee{r} say that, on DD,

  • θ\theta runs from 00 to π ⁣/4\nicefrac{\pi}{4} and

  • for each θ\theta in that range, rr runs from 00 to 2sinθ+cosθ\frac{2}{\sin\theta+\cos\theta}.

In Cartesian coordinates

  • θ=0\theta=0 is the positive xx-axis and

  • θ=π ⁣/4\theta=\nicefrac{\pi}{4} is the ray y=xy=x, x0x\ge 0 and

  • r=2sinθ+cosθr=\frac{2}{\sin\theta+\cos\theta}, or equivalently rcosθ+rsinθ=2r\cos\theta+r\sin\theta=2, is the line x+y=2x+y=2.

Looking at the sketch on the left below, we see that, since the lines y=xy=x and x+y=2x+y=2 cross at (1,1)(1,1),

D={ (x,y)  0y1, yx2y }\begin{align*} D=\Set{(x,y)}{0\le y\le 1,\ y\le x\le 2-y} \end{align*}

DD is the shaded region in the sketch on the right.

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

(c) Let DD denote the domain of integration. The symbols 02πdθ03cos2θ+9sin2θdr\int_0^{2\pi}\dee{\theta} \int_0^{\frac{3}{\sqrt{\cos^2\theta+9\sin^2\theta}}}\dee{r} say that, on DD,

  • θ\theta runs all the way from 00 to 2π2\pi and

  • for each θ\theta, rr runs from 00 to 3cos2θ+9sin2θ\frac{3}{\sqrt{\cos^2\theta+9\sin^2\theta}}.

In Cartesian coordinates

  • r=3cos2θ+9sin2θr=\frac{3}{\sqrt{\cos^2\theta+9\sin^2\theta}}, or equivalently r2cos2θ+9r2sin2θ=9r^2\cos^2\theta+9r^2\sin^2\theta=9, is the ellipse x2+9y2=9x^2+9y^2=9.

So DD is the interior of the ellipse x2+9y2=9x^2+9y^2=9 and DD is the shaded region in the sketch on the right.

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 820

Figure from prob_s3.2, line 806

Figure from prob_s3.2, line 806

2Stage 2Procedural

Practising the skill itself, until applying it is automatic.

Q7Stage 2

Use polar coordinates to evaluate each of the following integrals.

  1. S(x+y)dxdy\displaystyle\dblInt_S (x+y)\dee{x}\,\dee{y} where SS is the region in the first quadrant lying inside the disc x2+y2a2x^2+y^2\le a^2 and under the line y=3xy=\sqrt{3}x.

  2. Sx dxdy\displaystyle\dblInt_Sx\ \dee{x}\,\dee{y}, where SS is the disc segment x2+y22, x1x^2+y^2\le 2,\ x\ge 1.

  3. T(x2+y2)dxdy\displaystyle\dblInt_T (x^2+y^2)\dee{x}\,\dee{y} where TT is the triangle with vertices (0,0),(1,0)(0,0), (1,0) and (1,1)(1,1).

  4. x2+y21ln(x2+y2)dxdy\displaystyle\dblInt_{x^2+y^2\le 1} \ln(x^2+y^2)\,\dee{x}\,\dee{y}

Answer

(a) a36[3+1]\frac{a^3}{6}\big[\sqrt{3}+1\big] (b) 23\frac{2}{3} (c) 13\frac{1}{3} (d) π-\pi

Full solution

(a) In polar coordinates, the domain of integration, x2+y2a2x^2+y^2\le a^2, 0y3x0\le y\le \sqrt{3}x, becomes

0ra, 0rsinθ3rcosθ or 0ra, 0θarctan3=π3\begin{equation*} 0\le r\le a,\ 0\le r\sin\theta\le\sqrt{3}r\cos\theta\qquad\text{ or }\qquad 0\le r\le a,\ 0\le\theta\le \arctan\sqrt{3}=\frac{\pi}{3} \end{equation*}

The integral is

S(x+y)dxdy=0adr0π3dθ r(rcosθ+rsinθ)=0adr r2[sinθcosθ]0π3=a33[3212+1]=a36[3+1]\begin{align*} \dblInt_S (x+y)\dee{x}\,\dee{y} &=\int_0^a \dee{r}\int_0^{{\pi\over 3}}\dee{\theta}\ r\,(r\cos\theta+r\sin\theta)\\ &=\int_0^a \dee{r}\ r^2\Big[\sin\theta-\cos\theta\Big]_0^{{\pi\over 3}} =\frac{a^3}{3}\left[\frac{\sqrt{3}}{2}-\frac{1}{2}+1\right] =\frac{a^3}{6}\big[\sqrt{3}+1\big] \end{align*}

(b) In polar coordinates, the domain of integration, x2+y22x^2+y^2\le 2, x1x\ge 1,

Figure from prob_s3.2, line 953

Figure from prob_s3.2, line 953

becomes

r2, rcosθ1 or 1cosθr2\begin{equation*} r\le \sqrt{2},\ r\cos\theta\ge 1\qquad\text{ or }\qquad \frac{1}{\cos\theta}\le r\le\sqrt{2} \end{equation*}

For 1cosθr2\frac{1}{\cos\theta}\le r\le\sqrt{2} to be nonempty, we need cosθ12\cos\theta\le \frac{1}{\sqrt{2}} or θπ4|\theta|\le\frac{\pi}{4}. By symmetry under yyy\rightarrow -y, the integral is

Sx dxdy=20π4dθ1cosθ2dr r(rcosθ)=20π4dθ cosθ r331cosθ2=230π4dθ [23/2cosθ1cos2θ]=23[23/2sinθtanθ]0π4=23[23/2121]=23\begin{align*} \dblInt_Sx\ \dee{x}\,\dee{y} &=2\int_0^{{\pi\over 4}}\dee{\theta}\int_{1\over\cos\theta}^{\sqrt{2}} \dee{r}\ r\,(r\cos\theta)\\ &=2\int_0^{{\pi\over 4}}\dee{\theta}\ \cos\theta\ \frac{r^3}{3}\bigg|_{1\over\cos\theta}^{\sqrt{2}} =\frac{2}{3}\int_0^{{\pi\over 4}}\dee{\theta}\ \Big[2^{3/2}\cos\theta-\frac{1}{\cos^2\theta}\Big] \\ &=\frac{2}{3} \Big[2^{3/2}\sin\theta-\tan\theta\Big]_0^{{\pi\over 4}} =\frac{2}{3} \big[2^{3/2}\frac{1}{\sqrt{2}}-1\big] =\frac{2}{3} \end{align*}

(c) In polar coordinates, the triangle with vertices (0,0),(1,0)(0,0), (1,0) and (1,1)(1,1) has sides θ=0\theta=0, θ=π4\theta=\frac{\pi}{4} and r=1cosθr=\frac{1}{\cos\theta} (which is the polar coordinates version of x=1x=1). The integral is

T(x2+y2) dxdy=0π4dθ01cosθdr r(r2)=0π4dθ r4401cosθ=140π4dθ 1cos4θ=140π4dθ sec4θ=140π4dθ sec2θ(1+tan2θ)=1401dt (1+t2) where t=tanθ=14[t+t33]01=14 43=13\begin{align*} \dblInt_T (x^2+y^2)\ \dee{x}\,\dee{y} &=\int_0^{{\pi\over 4}}\dee{\theta}\int_0^{1\over\cos\theta} \dee{r}\ r(r^2)\\ &=\int_0^{{\pi\over 4}}\dee{\theta}\ \frac{r^4}{4}\bigg|_0^{1\over\cos\theta} =\frac{1}{4}\int_0^{{\pi\over 4}}\dee{\theta}\ \frac{1}{\cos^4\theta} =\frac{1}{4}\int_0^{{\pi\over 4}}\dee{\theta}\ \sec^4\theta\cr &=\frac{1}{4}\int_0^{{\pi\over 4}}\dee{\theta}\ \sec^2\theta\big(1+\tan^2\theta\big) =\frac{1}{4}\int_0^1d t\ \big(1+t^2\big)\text{ where }t=\tan\theta\cr &=\frac{1}{4}\left[t+\frac{t^3}{3}\right]_0^1 =\frac{1}{4}\ \frac{4}{3} =\frac{1}{3} \end{align*}

(d) In polar coordinates, the domain of integration, x2+y21x^2+y^2\le 1, becomes 0r10\le r\le 1, 0θ2π0\le\theta\le 2\pi. So

x2+y21ln(x2+y2)dxdy=02πdθ01dr rlnr2=2π01dr rlnr2=π01ds lns where s=r2=π[slnss]01=π\begin{align*} \dblInt_{x^2+y^2\le 1}\hskip-5pt \ln(x^2+y^2)\,\dee{x}\,\dee{y} &=\int_0^{2\pi}\hskip-3pt \dee{\theta}\int_0^1\dee{r}\ r\ln r^2 =2\pi\int_0^1\dee{r}\ r\ln r^2 =\pi\int_0^1 \dee{s}\ \ln s\text{ where }s=r^2\cr &=\pi\Big[s\ln s-s\Big]_0^1 =-\pi \end{align*}

To be picky, lns\ln s tends to -\infty as ss tends to 00. So 01dslns\int_0^1\dee{s}\,\ln s is an improper integral. The careful way to evaluate it is

01ds lns=limε0+ε1ds lns=limε0+[slnss]ε1=limε0+[1εlnε+ε]=1\begin{align*} \int_0^1 \dee{s}\ \ln s &=\lim_{\veps\to 0^+}\int_\veps^1 \dee{s}\ \ln s =\lim_{\veps\to 0^+}\Big[s\ln s-s\Big]_\veps^1 =\lim_{\veps\to 0^+}\Big[-1-\veps\ln\veps+\veps\Big] =-1 \end{align*}

That limε0+εlnε=0\lim\limits_{\veps\to 0^+}\veps\ln\veps = 0 was shown in Example 3.7.15 of the CLP-1 text.

Q8Stage 2

Find the volume lying inside the sphere x2+y2+z2=2x^2+y^2+z^2=2 and above the paraboloid z=x2+y2z=x^2+y^2.

Answer

π[43276]2.26\pi \left[\frac{4}{3}\sqrt{2}-\frac{7}{6}\right] \approx 2.26

Full solution

The top surface x2+y2+z2=2x^2+y^2+z^2=2 meets the bottom surface z=x2+y2z=x^2+y^2 when zz obeys x2+y2=z=2z2x^2+y^2=z=2-z^2. That is, when 0=z2+z2=(z1)(z+2)0=z^2+z-2=(z-1)(z+2). The root z=2z=-2 is inconsistent with z=x2+y20z=x^2+y^2\ge 0. So the top and bottom surfaces meet at the circle z=1z=1, x2+y2=1x^2+y^2=1.

In polar coordinates, the top surface is z2=2r2z^2=2-r^2, or equivalently z=2r2z=\sqrt{2-r^2}, and the bottom surface is z=r2z=r^2. So the height of the volume above the point with polar coordinates (r,θ)(r,\theta) is 2r2r2\sqrt{2-r^2}-r^2 and

Volume=01dr02πdθ r[2r2r2]=2π01dr r[2r2r2]=2π[13(2r2)3/2r44]01=2π[1314+1323/2]=π[43276]2.26\begin{align*} \text{Volume}&=\int_0^1\dee{r}\int_0^{2\pi} \dee{\theta}\ r\,\big[\sqrt{2-r^2}-r^2\big] =2\pi \int_0^1\dee{r}\ r\,\big[\sqrt{2-r^2}-r^2\big]\\ &=2\pi \left[-\frac{1}{3}{(2-r^2)}^{3/2}-\frac{r^4}{4}\right]_0^1 =2\pi \left[-\frac{1}{3}-\frac{1}{4}+\frac{1}{3}2^{3/2}\right] \\ &=\pi \left[\frac{4}{3}\sqrt{2}-\frac{7}{6}\right] \approx 2.26 \end{align*}

In Cartesian coordinates

Volume=401dx01x2dy [2x2y2x2y2]\begin{align*} \text{Volume}&=4\int_0^1\dee{x}\int_0^{\sqrt{1-x^2}} \dee{y}\ \big[\sqrt{2-x^2-y^2}-x^2-y^2\big] \end{align*}

The yy integral can be done using the substitution y=2x2costy=\sqrt{2-x^2}\cos t, but it is easier to use polar coordinates.

Q9Stage 2

Let a>0a>0. Find the volume lying inside the cylinder x2+(ya)2=a2x^2+(y-a)^2=a^2 and between the upper and lower halves of the cone z2=x2+y2z^2=x^2+y^2.

Answer

649a3\frac{64}{9}a^3

Full solution

For this region xx and yy run over the interior of the cylinder x2+(ya)2=a2x^2+(y-a)^2=a^2. For each (x,y)(x,y) inside the cylinder, zz runs from x2+y2-\sqrt{x^2+y^2} to x2+y2\sqrt{x^2+y^2}. As x2+(ya)2=a2x^2+(y-a)^2=a^2 if and only if x2+y22ay=0x^2+y^2-2ay=0, the cylinder has equation r2=2arsinθr^2=2ar\sin\theta, or equivalently, r=2asinθr=2a\sin\theta, in polar coordinates.

Figure from prob_s3.2, line 1102

Figure from prob_s3.2, line 1102

Thus (r,θ)(r,\theta) runs over 0θπ, 0r2asinθ0\le\theta\le\pi,\ 0\le r\le 2a\sin\theta and for each (r,θ)(r,\theta) in this region zz runs from r-r to rr. By symmetry under xxx\rightarrow -x, the volume is

Volume=20π2dθ02asinθdr r[r(r)]=40π2dθ02asinθdr r2=430π2 ⁣ ⁣dθ (2asinθ)3=323a30π2 ⁣ ⁣dθ sinθ(1cos2θ)=323a310dt (1t2) where t=cosθ=323a3[tt33]10=649a3\begin{align*} \text{Volume} &=2\int_0^{{\pi\over 2}}\dee{\theta}\int_0^{2a\sin\theta}\dee{r}\ r\big[r-(-r)\big] =4\int_0^{{\pi\over 2}}\dee{\theta}\int_0^{2a\sin\theta}\dee{r}\ r^2 =\frac{4}{3}\int_0^{{\pi\over 2}}\!\!\dee{\theta}\ (2a\sin\theta)^3 \\ &=\frac{32}{3}a^3\int_0^{{\pi\over 2}}\!\!\dee{\theta}\ \sin\theta(1-\cos^2\theta) =-\frac{32}{3}a^3\int_1^0 dt\ (1-t^2)\text{ where }t=\cos\theta\cr &=-\frac{32}{3}a^3\left[t-\frac{t^3}{3}\right]_1^0 =\frac{64}{9}a^3 \end{align*}
Q10Stage 2

Let a>0a>0. Find the volume common to the cylinders x2+y22axx^2+y^2\le 2ax and z22axz^2\le 2ax.

Answer

12815a3\frac{128}{15}a^3

Full solution

The figure below shows the top view of the specified solid. (x,y)(x,y) runs over the interior of the circle x2+y2=2axx^2+y^2=2ax. For each fixed (x,y)(x,y) in this disk, zz runs from 2ax-\sqrt{2ax} to +2ax+\sqrt{2ax}. In polar coordinates, the circle is r2=2arcosθr^2=2ar\cos\theta or r=2acosθr=2a\cos\theta.

Figure from prob_s3.2, line 1146

Figure from prob_s3.2, line 1146

The solid is symmetric under yyy\rightarrow -y and zzz\rightarrow -z, so we can restrict to y0y\ge 0, z0z\ge 0 and multiply by 4. The volume is

Volume=40π2dθ02acosθdr r2arcosθ=40π2dθ 2acosθ 25 r5/202acosθ=850π2dθ (2acosθ)3=645a30π2dθ cosθ(1sin2θ)=645a301dt (1t2) where t=sinθ=645a3[tt33]01=12815a3\begin{align*} \text{Volume} &=4\int_0^{\pi\over 2} \dee{\theta}\int_0^{2a\cos\theta} \dee{r}\ r\sqrt{2ar\cos\theta} \\ &=4\int_0^{\pi\over 2} \dee{\theta}\ \sqrt{2a\cos\theta}\ \frac{2}{5}\ r^{5/2}\bigg|_0^{2a\cos\theta} \\ &=\frac{8}{5}\int_0^{\pi\over 2} \dee{\theta}\ \big(2a\cos\theta\big)^3 =\frac{64}{5}a^3\int_0^{\pi\over 2} \dee{\theta}\ \cos\theta\big(1-\sin^2\theta\big)\cr &=\frac{64}{5}a^3\int_0^1 dt\ \big(1-t^2\big) \qquad\text{ where }t=\sin\theta\cr &=\frac{64}{5}a^3\left[t-\frac{t^3}{3}\right]_0^1 =\frac{128}{15}a^3 \end{align*}
Q11Stage 2Past exam · M200 2005D

Consider the region EE in 3–dimensions specified by the inequalities x2+y22yx^2 + y^2 \le 2y and 0zx2+y20 \le z \le \sqrt{x^2 + y^2}.

  1. Draw a reasonably accurate picture of EE in 3–dimensions. Be sure to show the units on the coordinate axes.

  2. Use polar coordinates to find the volume of EE. Note that you will be “using polar coordinates” if you solve this problem by means of cylindrical coordinates.

    Hint:
    sinnu du=1nsinn1u cosu+n1nsinn2u du\int \sin^n u\ \dee{u} =-\frac{1}{n}\sin^{n-1}u\ \cos u +\frac{n-1}{n}\int\sin^{n-2}u\ \dee{u}

Answer

(a)

Figure from prob_s3.2, line 1200

Figure from prob_s3.2, line 1200

(b) 329\frac{32}{9}

Full solution

(a)

  • The equation x2+y22yx^2 + y^2 \le 2y is equivalent to the equation x2+(y1)2=1x^2 + (y-1)^2=1, which is the equation of the cylinder whose z=z0z=z_0 cross–section is the horizontal circle of radius 11, centred on x=0x=0, y=1y=1, z=z0z=z_0. The part of this cylinder in the first octant is sketched in the figure on the left below.

  • zx2+y2z \le \sqrt{x^2 + y^2} is the equation of the cone with vertex (0,0,0)(0,0,0), and axis the positive zz–axis, whose radius at height z=2z=2 is 22. The part of this cone in the first octant is sketched in the figure on the right below.

Figure from prob_s3.2, line 1209

Figure from prob_s3.2, line 1209

Figure from prob_s3.2, line 1209

Figure from prob_s3.2, line 1209

The region EE is the part of the cylinder that is above the xyxy–plane (since z0z\ge 0) outside the cone (since zx2+y2z\le\sqrt{x^2+y^2}). The part of EE that is in the first octant is outlined in red in the figure below. Both x2+y22yx^2 + y^2 \le 2y and 0zx2+y20 \le z \le \sqrt{x^2 + y^2} are invariant under xxx\rightarrow -x. So EE is also invariant under xxx\rightarrow -x. That is, EE is symmetric about the yzyz–plane and contains, in the octant x0x\le 0, y0y\ge 0, z0z\ge 0, a mirror image of the first octant part of EE.

Figure from prob_s3.2, line 1209

Figure from prob_s3.2, line 1209

(b) In polar coordinates, x2+y22yx^2 + y^2 \le 2y becomes

r22rsinθ    r2sinθ\begin{equation*} r^2\le 2r\sin\theta \iff r\le 2\sin\theta \end{equation*}

Let us denote by DD the base region of the part of EE in the first octant (i.e. the shaded region in the figure above). Think of DD as being part of the xyxy–plane. In polar coordinates, on DD

  • θ\theta runs from 00 to π2\frac{\pi}{2}. (Recall that DD is contained in the first quadrant.)

  • For each θ\theta in that range, rr runs from 00 to 2sinθ2\sin\theta.

Because

  • in polar coordinates dA=rdrdθ\dee{A} = r\,\dee{r}\,\dee{\theta}, and

  • the height of EE above each point (x,y)(x,y) in DD is x2+y2\sqrt{x^2+y^2}, or, in polar coordinates, rr, and

  • the volume of EE is twice the volume of the part of EE in the first octant,

we have

Volume(E)=20π2dθ02sinθdr r2=1630π2dθ sin3θ=1630π2dθ sinθ (1cos2θ)=16310du (1u2)with u=cosθ, du=sinθ dθ=163[113]=329\begin{align*} \text{Volume}(E) &= 2\int_0^{\frac{\pi}{2}}\dee{\theta} \int_0^{2\sin\theta}\dee{r}\ r^2 \\ &=\frac{16}{3} \int_0^{\frac{\pi}{2}}\dee{\theta}\ \sin^3\theta =\frac{16}{3} \int_0^{\frac{\pi}{2}}\dee{\theta}\ \sin\theta\ \big(1-\cos^2\theta\big) \\ &=-\frac{16}{3} \int_1^0\dee{u}\ \big(1-u^2\big)\qquad \text{with }u=\cos\theta,\ \dee{u}=-\sin\theta\ \dee{\theta} \\ &=\frac{16}{3}\left[1-\frac{1}{3}\right] \\ &=\frac{32}{9} \end{align*}
Q12Stage 2Past exam · M200 2006A

Evaluate the iterated double integral

x=0x=2y=0y=4x2(x2+y2)32 dydx\begin{equation*} \int_{x=0}^{x=2}\int_{y=0}^{y=\sqrt{4-x^2}} {(x^2+y^2)}^{\frac{3}{2}}\ \dee{y}\,\dee{x} \end{equation*}
Answer

16π5\frac{16\pi}{5}

Full solution

On the domain of integration

  • xx runs for 00 to 22, and

  • for each fixed xx in that range, yy runs from 00 to 4x2\sqrt{4-x^2}. The equation y=4x2y=\sqrt{4-x^2} is equivalent to x2+y2=4x^2+y^2=4, y0y\ge 0.

This domain is sketched in the figure on the left below.

Figure from prob_s3.2, line 1301

Figure from prob_s3.2, line 1301

Figure from prob_s3.2, line 1301

Figure from prob_s3.2, line 1301

Considering that

  • the integrand, (x2+y2)32{(x^2+y^2)}^{\frac{3}{2}}, is invariant under rotations about the origin and

  • the outer curve, x2+y2=4x^2+y^2=4, is invariant under rotations about the origin

we'll use polar coordinates. In polar coordinates,

  • the outer curve, x2+y2=4x^2+y^2=4, is r=2r=2, and

  • the integrand, (x2+y2)32{(x^2+y^2)}^{\frac{3}{2}} is r3r^3, and

  • dA=rdrdθ\dee{A}=r\,\dee{r}\,\dee{\theta}

Looking at the figure on the right above, we see that the given integral is, in polar coordinates,

0π/2dθ02dr r(r3)=π2 255=16π5\begin{align*} \int_0^{\pi/2}\dee{\theta}\int_0^2\dee{r}\ r (r^3) &=\frac{\pi}{2}\ \frac{2^5}{5} =\frac{16\pi}{5} \end{align*}
Q13Stage 2Past exam · M200 2006D
  1. Sketch the region L\cL (in the first quadrant of the xyxy–plane) with boundary curves

    x2+y2=2, x2+y2=4, y=x, y=0.\begin{equation*} x^2 + y^2 = 2,\ x^2 + y^2 = 4,\ y = x,\ y = 0. \end{equation*}

    The mass of a thin lamina with a density function ρ(x,y)\rho(x,y) over the region L\cL is given by

    M=Lρ(x,y)dA\begin{equation*} M =\dblInt_\cL \rho(x,y)\,\dee{A} \end{equation*}
  2. Find an expression for MM as an integral in polar coordinates.

  3. Find M when

    ρ(x,y)=2xyx2+y2\begin{equation*} \rho(x,y) = \frac{2xy}{x^2+y^2} \end{equation*}
Answer

(a)

Figure from prob_s3.2, line 1376

Figure from prob_s3.2, line 1376

(b) M=0π/4dθ22dr rρ(rcosθ,rsinθ)M = \int_0^{\pi/4}\dee{\theta}\int_{\sqrt{2}}^2\dee{r}\ r\, \rho(r\cos\theta\,,\,r\sin\theta) (c) 12\frac{1}{2}

Full solution

(a) The region L\cL is sketched in the figure on the leflt below.

Figure from prob_s3.2, line 1376

Figure from prob_s3.2, line 1376

Figure from prob_s3.2, line 1388

Figure from prob_s3.2, line 1388

(b) In polar coordinates

  • the circle x2+y2=2x^2+y^2=2 is r2=2r^2=2 or r=2r=\sqrt{2}, and

  • the circle x2+y2=4x^2+y^2=4 is r2=4r^2=4 or r=2r=2, and

  • the line y=xy=x is rsinθ=rcosθr\sin\theta = r\cos\theta, or tanθ=1\tan\theta =1, or (for the part in the first quadrant) θ=π4\theta=\frac{\pi}{4}, and

  • the positive xx–axis (y=0y=0, x0x\ge 0) is θ=0\theta=0

Looking at the figure on the right above, we see that, in L\cL,

  • θ\theta runs from 00 to π4\frac{\pi}{4}, and

  • for each fixed θ\theta in that range, rr runs from 2\sqrt{2} to 22.

  • dA\dee{A} is rdrdθr\,\dee{r}\,\dee{\theta}

So

M=0π/4dθ22dr rρ(rcosθ,rsinθ)\begin{align*} M = \int_0^{\pi/4}\dee{\theta}\int_{\sqrt{2}}^2\dee{r}\ r\, \rho(r\cos\theta\,,\,r\sin\theta) \end{align*}

(c) When

ρ=2xyx2+y2=2r2cosθsinθr2=sin(2θ)\begin{align*} \rho = \frac{2xy}{x^2+y^2} = \frac{2r^2\cos\theta\,\sin\theta}{r^2} =\sin(2\theta) \end{align*}

we have

M=0π/4dθ22dr rsin(2θ)=[0π/4sin(2θ) dθ][22r dr]=[12cos(2θ)]0π/4[r22]22=12 422=12\begin{align*} M &= \int_0^{\pi/4}\dee{\theta}\int_{\sqrt{2}}^2\dee{r}\ r\, \sin(2\theta) \\ &=\left[\int_0^{\pi/4}\sin(2\theta)\ \dee{\theta}\right] \left[\int_{\sqrt{2}}^2 r\ \dee{r}\right] \\ &=\left[-\frac{1}{2}\cos(2\theta)\right]_0^{\pi/4} \left[ \frac{r^2}{2}\right]_{\sqrt{2}}^2 =\frac{1}{2}\ \frac{4-2}{2} \\ &=\frac{1}{2} \end{align*}
Q14Stage 2Past exam · M200 2009A

Evaluate R21(1+x2+y2)2 dA\displaystyle \dblInt_{\bbbr^2} \frac{1}{{(1+x^2+y^2)}^2}\ \dee{A}.

Answer

π\pi

Full solution

We'll use polar coordinates. The domain of integration is

R2={ (rcosθ,rsinθ)  0r<, 0θ2π }\begin{equation*} \bbbr^2=\Set{(r\cos\theta\,,\,r\sin\theta)}{0\le r<\infty,\ 0\le\theta\le 2\pi} \end{equation*}

The given integral is improper, so we'll start by integrating rr from 00 to an arbitrary R>0R>0, and then we'll take the limit RR\rightarrow\infty. In polar coordinates, the integrand 1(1+x2+y2)2=1(1+r2)2\frac{1}{{(1+x^2+y^2)}^2}=\frac{1}{{(1+r^2)}^2}, and dA=rdrdθ\dee{A}=r\,\dee{r}\,\dee{\theta}, so

R21(1+x2+y2)2 dA=limR02πdθ0Rdrr(1+r2)2=limR02πdθ [12(1+r2)]0R=limR2π[1212(1+R2)]=π\begin{align*} \dblInt_{\bbbr^2} \frac{1}{{(1+x^2+y^2)}^2}\ \dee{A} &=\lim_{R\rightarrow\infty} \int_0^{2\pi}\dee{\theta}\int_0^R\dee{r} \frac{r}{{(1+r^2)}^2} \\ &=\lim_{R\rightarrow\infty} \int_0^{2\pi}\dee{\theta}\ \left[-\frac{1}{2(1+r^2)}\right]_0^R \\ &=\lim_{R\rightarrow\infty} 2\pi \left[\frac{1}{2}-\frac{1}{2(1+R^2)}\right] \\ &=\pi \end{align*}
Q15Stage 2Past exam · M200 2011D

Evaluate the double integral

Dyx2+y2dA\begin{equation*} \dblInt_D y\sqrt{x^2+y^2}\,\dee{A} \end{equation*}

over the region D={ (x,y)  x2+y22, 0yx }D =\Set{(x,y)}{ x^2+y^2\le 2,\ 0\le y\le x}.

Answer

1121-\frac{1}{\sqrt{2}}

Full solution

Let's switch to polar coordinates. In polar coordinates, the circle x2+y2=2x^2+y^2=2 is r=2r=\sqrt{2} and the line y=xy=x is θ=π4\theta=\frac{\pi}{4}.

Figure from prob_s3.2, line 1495

Figure from prob_s3.2, line 1495

In polar coordinates dA=rdrdθ\dee{A} = r\,\dee{r}\,\dee{\theta}, so the integral

Dyx2+y2dA=0π/4dθ02dr r rsinθy rx2+y2=0π/4dθ sinθ [r44]02=[cosθ]0π/4=112\begin{align*} \dblInt_D y\sqrt{x^2+y^2}\,\dee{A} &=\int_0^{\pi/4}\dee{\theta}\int_0^{\sqrt{2}}\dee{r}\ r\ \overbrace{r\sin\theta}^{y}\ \overbrace{r}^{\sqrt{x^2+y^2}} \\ &=\int_0^{\pi/4}\dee{\theta}\ \sin\theta\ \left[\frac{r^4}{4}\right]_0^{\sqrt{2}} \\ &=\Big[-\cos\theta\Big]_0^{\pi/4} \\ &= 1-\frac{1}{\sqrt{2}} \end{align*}
Q16Stage 2Past exam · M200 2013D

This question is about the integral

013y4y2ln(1+x2+y2) dxdy\begin{equation*} \int_0^1 \int_{\sqrt{3}y}^{\sqrt{4-y^2}} \ln\big(1+x^2+y^2)\ \dee{x}\,\dee{y} \end{equation*}
  1. Sketch the domain of integration.

  2. Evaluate the integral by transforming to polar coordinates.

Answer

(a)

Figure from prob_s3.2, line 1532

Figure from prob_s3.2, line 1532

(b) π12[5ln(5)4]\frac{\pi}{12}\big[5\ln(5)-4\big]

Full solution

(a) On the domain of integration

  • yy runs from 00 to 11. In inequalities, 0y10\le y\le 1.

  • For each fixed yy in that range, xx runs from 3y\sqrt{3}\,y to 4y2\sqrt{4-y^2}. In inequalities, that is 3yx4y2\sqrt{3}\,y\le x\le \sqrt{4-y^2}. Note that the inequalities x4y2x\le \sqrt{4-y^2}, x0x\ge 0 are equivalent to x2+y24x^2+y^2\le 4, x0x\ge 0.

Note that the line x=3yx=\sqrt{3}\, y and the circle x2+y24x^2+y^2\le 4 intersect when 3y2+y2=43y^2+y^2=4, i.e. y=±1y=\pm 1. Here is a sketch.

Figure from prob_s3.2, line 1541

Figure from prob_s3.2, line 1541

(b) In polar coordinates, the circle x2+y2=4x^2+y^2= 4 is r=2r=2 and the line x=3yx=\sqrt{3}\, y, i.e. yx=13\frac{y}{x} =\frac{1}{\sqrt{3}}, is tanθ=13\tan\theta=\frac{1}{\sqrt{3}} or θ=π6\theta=\frac{\pi}{6}. As dxdy=rdrdθ\dee{x}\,\dee{y} = r\,\dee{r}\,\dee{\theta}, the domain of integration is

{ (rcosθ,rsinθ)  0θπ ⁣/6, 0r2 }\begin{align*} \Set{(r\cos\theta,r\sin\theta)}{0\le \theta\le\nicefrac{\pi}{6},\ 0\le r\le 2} \end{align*}

and

013y4y2ln(1+x2+y2) dxdy=02dr0π/6dθ rln(1+r2)=π602dr rln(1+r2)=π1215duln(u)with u=1+r2, du=2rdr=π12[uln(u)u]15=π12[5ln(5)4]\begin{align*} \int_0^1 \int_{\sqrt{3}y}^{\sqrt{4-y^2}} \ln\big(1+x^2+y^2)\ \dee{x}\,\dee{y} &= \int_0^2\dee{r}\int_0^{\pi/6}\dee{\theta}\ r\,\ln(1+r^2) = \frac{\pi}{6}\int_0^2\dee{r}\ r\,\ln(1+r^2) \\ &=\frac{\pi}{12}\int_1^5 \dee{u} \ln(u) \qquad\text{with }u=1+r^2,\ \dee{u}=2r\,\dee{r} \\ &=\frac{\pi}{12}\Big[u\ln(u)-u\Big]_1^5 \\ &=\frac{\pi}{12}\big[5\ln(5)-4\big] \end{align*}
Q17Stage 2Past exam · M200 2014A

Let DD be the region in the xyxy–plane bounded on the left by the line x=2x = 2 and on the right by the circle x2+y2=16x^2 + y^2 = 16. Evaluate

D(x2+y2)3/2 dA\begin{equation*} \dblInt_D\big(x^2+y^2\big)^{-3/2}\ \dee{A} \end{equation*}
Answer

32π6\frac{\sqrt{3}}{2}-\frac{\pi}{6}

Full solution

Here is a sketch of DD.

Figure from prob_s3.2, line 1598

Figure from prob_s3.2, line 1598

We'll use polar coordinates. In polar coordinates the circle x2+y2=16x^2+y^2=16 is r=4r=4 and the line x=2x=2 is rcosθ=2r\cos\theta =2. So

D={(rcosθ,rsinθ)  π3θπ3, 2cosθr4 }\begin{align*} D = \left\{(r\cos\theta\,,\,r\sin\theta)\ \left|\ -\frac{\pi}{3}\le\theta\le\frac{\pi}{3},\ \frac{2}{\cos\theta}\le r\le 4\ \right.\right\} \end{align*}

and, as dA=rdrdθ\dee{A} = r\,\dee{r}\,\dee{\theta}, the specified integral is

D(x2+y2)3/2 dA=π/3π/3dθ2/cosθ4dr r1r3=π/3π/3dθ [1r]2/cosθ4=π/3π/3dθ [cosθ214]=[sinθ2θ4]π/3π/3=32π6\begin{align*} \dblInt_D\big(x^2+y^2\big)^{-3/2}\ \dee{A} &= \int_{-\pi/3}^{\pi/3} \dee{\theta}\int_{2/\cos\theta}^4\dee{r}\ r\frac{1}{r^3} \\ &= \int_{-\pi/3}^{\pi/3} \dee{\theta}\ \left[-\frac{1}{r}\right]_{2/\cos\theta}^4 \\ &= \int_{-\pi/3}^{\pi/3} \dee{\theta}\ \left[\frac{\cos\theta}{2}-\frac{1}{4}\right] \\ &= \left[\frac{\sin\theta}{2}-\frac{\theta}{4}\right]_{-\pi/3}^{\pi/3} \\ &=\frac{\sqrt{3}}{2}-\frac{\pi}{6} \end{align*}
Q18Stage 2Past exam · M200 2014D

In the xyxy–plane, the disk x2+y22xx^2 + y^2 \le 2x is cut into 22 pieces by the line y=xy = x. Let DD be the larger piece.

  1. Sketch DD including an accurate description of the center and radius of the given disk. Then describe DD in polar coordinates (r,θ)(r, \theta).

  2. Find the volume of the solid below z=x2+y2z = \sqrt{x^2 + y^2} and above DD.

Answer

(a) D={ (rcosθ,rsinθ)  π ⁣/2θπ ⁣/4, 0r2cosθ }D = \Set{(r\cos\theta\,,\,r\sin\theta)} {-\nicefrac{\pi}{2}\le\theta\le\nicefrac{\pi}{4},\ 0\le r\le 2\cos\theta}

(b) Volume=40182+169\text{Volume}=\frac{40}{18\sqrt{2}} +\frac{16}{9}

Full solution

(a) The inequality x2+y22xx^2 + y^2 \le 2x is equivalent to (x1)2+y21(x-1)^2 + y^2 \le 1 and says that (x,y)(x,y) is to be inside the disk of radius 11 centred on (1,0)(1,0). Here is a sketch.

Figure from prob_s3.2, line 1649

Figure from prob_s3.2, line 1649

In polar coordinates, x=rcosθx=r\cos\theta, y=rsinθy=r\sin\theta so that the line y=xy=x is θ=π4\theta=\frac{\pi}{4} and the circle x2+y2=2xx^2+y^2=2x is

r2=2rcosθorr=2cosθ\begin{equation*} r^2=2r\cos\theta \qquad\text{or}\qquad r=2\cos\theta \end{equation*}

Consequently

D={ (rcosθ,rsinθ)  π ⁣/2θπ ⁣/4, 0r2cosθ }\begin{equation*} D = \Set{(r\cos\theta\,,\,r\sin\theta)} {-\nicefrac{\pi}{2}\le\theta\le\nicefrac{\pi}{4},\ 0\le r\le 2\cos\theta} \end{equation*}

(b) The solid has height z=rz=r above the point in DD with polar coordinates rr, θ\theta. So the

Volume=Dr dA=Dr2 drdθ=π/2π/4dθ02cosθdr r2=83π/2π/4dθ cos3θ=83π/2π/4dθ cosθ[1sin2θ]=83[sinθsin3θ3]π/2π/4=83[(12162)(1+13)]=40182+169\begin{align*} \text{Volume} &= \dblInt_D r\ \dee{A}=\dblInt_D r^2\ \dee{r}\, \dee{\theta} =\int_{-\pi/2}^{\pi/4}\dee{\theta}\int_0^{2\cos\theta} \dee{r}\ r^2 \\ &= \frac{8}{3}\int_{-\pi/2}^{\pi/4}\dee{\theta}\ \cos^3\theta = \frac{8}{3}\int_{-\pi/2}^{\pi/4}\dee{\theta}\ \cos\theta\big[1-\sin^2\theta\big] \\ &=\frac{8}{3} \left[\sin\theta -\frac{\sin^3\theta}{3}\right]_{-\pi/2}^{\pi/4}\\ &=\frac{8}{3}\left[\left(\frac{1}{\sqrt{2}} -\frac{1}{6\sqrt{2}}\right) -\left(-1 + \frac{1}{3}\right) \right] \\ &=\frac{40}{18\sqrt{2}} +\frac{16}{9} \end{align*}
Q19Stage 2Past exam · M200 2000A

Let DD be the shaded region in the diagram. Find the average distance of points in DD from the origin. You may use that cosn(x)dx=cosn1(x)sin(x)n+n1ncosn2(x)dx\int\cos^n(x)\,dx = \frac{\cos^{n-1}(x)\sin(x)}{n} +\frac{n-1}{n}\int\cos^{n-2}(x)\,dx for all natural numbers n2n\ge 2.

Figure from prob_s3.2, line 1687

Figure from prob_s3.2, line 1687

Answer

2π+44/9π+81.4422\frac{\pi+44/9}{\pi+8}\approx 1.442

Full solution

We'll use polar coordinates. In DD

  • θ\theta runs from 00 to π2\frac{\pi}{2} and

  • for each fixed θ\theta between 00 and π2\frac{\pi}{2}, rr runs from 11 to 1+cos(θ)1+\cos(\theta).

So the area of DD is

area=A=0π/2dθ11+cosθdr r=0π/2dθ 12r211+cosθ=0π/2dθ [12cos2θ+cosθ]\begin{equation*} \text{area}=A=\int_0^{\pi/2} \dee{\theta}\int_1^{1+\cos\theta} \dee{r}\ r =\int_0^{\pi/2} \dee{\theta}\ \frac{1}{2} r^2\bigg|_1^{1+\cos\theta} =\int_0^{\pi/2} \dee{\theta}\ \left[\frac{1}{2} \cos^2\theta+\cos\theta\right] \end{equation*}

We are interested in the average value of rr on DD, which is

ave dist=1A0π/2dθ11+cosθdr r2=1A0π/2dθ 13r311+cosθ=1A0π/2dθ [13cos3θ+cos2θ+cosθ]\begin{align*} \text{ave\ dist}&=\frac{1}{A}\int_0^{\pi/2} \dee{\theta}\int_1^{1+\cos\theta} \dee{r}\ r^2 =\frac{1}{A}\int_0^{\pi/2} \dee{\theta}\ \frac{1}{3} r^3\bigg|_1^{1+\cos\theta} \\ &=\frac{1}{A}\int_0^{\pi/2} \dee{\theta}\ \left[\frac{1}{3} \cos^3\theta +\cos^2\theta+\cos\theta\right] \end{align*}

Now we evaluate the integrals of the various powers of cosine.

0π/2cosθ dθ=sinθ0π/2=10π/2cos2θ dθ=cosθsinθ20π/2+120π/2dθ=π40π/2cos3θ dθ=cos2θsinθ30π/2+230π/2cosθ dθ=23\begin{align*} \int_0^{\pi/2}\cos\theta\ \dee{\theta}&=\sin\theta\,\bigg|_0^{\pi/2}=1 \\ \int_0^{\pi/2}\cos^2\theta\ \dee{\theta}&=\frac{\cos\theta\sin\theta}{2}\,\bigg|_0^{\pi/2} +\frac{1}{2}\int _0^{\pi/2}\dee{\theta}=\frac{\pi}{4}\cr \int_0^{\pi/2}\cos^3\theta\ \dee{\theta}&=\frac{\cos^2\theta\sin\theta}{3}\,\bigg|_0^{\pi/2} +\frac{2}{3}\int _0^{\pi/2}\cos\theta\ \dee{\theta}=\frac{2}{3}\cr \end{align*}

So A=π8+1A=\frac{\pi}{8}+1 and

ave dist=8π+8[29+π4+1]=2π+44/9π+81.442\begin{align*} \text{ave\ dist}=\frac{8}{\pi+8}\left[\frac{2}{9}+\frac{\pi}{4}+1\right] =2\frac{\pi+44/9}{\pi+8}\approx 1.442 \end{align*}

3Stage 3Application

Further than practice: several ideas at once, or an unfamiliar situation.

Q20Stage 3Past exam · M200 2010A

Let GG be the region in R2\bbbr^2 given by

x2+y210x2yy2x\begin{gather*} x^2 + y^2 \le 1 \\ 0 \le x \le 2y \\ y \le 2x \end{gather*}
  1. Sketch the region GG.

  2. Express the integral Gf(x,y) dA\dblInt_G f(x,y)\ \dee{A} a sum of iterated integrals f(x,y) dxdy\dblInt f(x, y)\ \dee{x}\dee{y}.

  3. Express the integral Gf(x,y) dA\dblInt_G f(x,y)\ \dee{A} as an iterated integral in polar coordinates (r,θ)(r, \theta) where x=rcos(θ)x = r \cos(\theta) and y=rsin(θ)y = r \sin(\theta).

Answer

(a)

Figure from prob_s3.2, line 1775

Figure from prob_s3.2, line 1775

(b)

Gf(x,y) dA=015dyy/22ydx f(x,y)+1525dyy/21y2dx f(x,y)\begin{align*} \dblInt_G f(x,y)\ \dee{A} &=\int_0^{\frac{1}{\sqrt{5}}}\dee{y}\int_{y/2}^{2y}\dee{x}\ f(x,y) +\int_{\frac{1}{\sqrt{5}}}^{\frac{2}{\sqrt{5}}}\dee{y}\int_{y/2}^{\sqrt{1-y^2}} \dee{x}\ f(x,y) \end{align*}

(c)

Gf(x,y) dA=arctan12arctan2dθ01dr rf(rcosθ,rsinθ)\begin{align*} \dblInt_G f(x,y)\ \dee{A} &=\int_{\arctan\frac{1}{2}}^{\arctan 2}\dee{\theta} \int_0^1\dee{r}\ r\,f(r\cos\theta,r\sin\theta) \end{align*}
Full solution

(a) Observe that

  • the condition x2+y21x^2+y^2\le 1 restricts GG to the interior of the circle of radius 11 centred on the origin, and

  • the conditions 0x2y0\le x\le 2y restricts GG to x0x\ge 0, y0y\ge 0, i.e. to the first quadrant, and

  • the conditions x2yx\le 2y and y2xy\le 2x restrict x2y2x\frac{x}{2}\le y\le 2x. So GG lies below the (steep) line y=2xy=2x and lies above the (not steep) line y=x2y=\frac{x}{2}.

Here is a sketch of GG

Figure from prob_s3.2, line 1775

Figure from prob_s3.2, line 1775

(b) Observe that the line y=2xy=2x crosses the circle x2+y2=1x^2+y^2=1 at a point (x,y)(x,y) obeying

x2+(2x)2=x2+y2=1    5x2=1\begin{align*} x^2+(2x)^2=x^2+y^2=1 \implies 5x^2=1 \end{align*}

and that the line x=2yx=2y crosses the circle x2+y2=1x^2+y^2=1 at a point (x,y)(x,y) obeying

(2y)2+y2=x2+y2=1    5y2=1\begin{align*} (2y)^2+y^2=x^2+y^2=1 \implies 5y^2=1 \end{align*}

So the intersection point of y=2xy=2x and x2+y2=1x^2+y^2=1 in the first octant is (15,25)\left(\frac{1}{\sqrt{5}}\,,\,\frac{2}{\sqrt{5}}\right) and the intersection point of x=2yx=2y and x2+y2=1x^2+y^2=1 in the first octant is (25,15)\left(\frac{2}{\sqrt{5}}\,,\,\frac{1}{\sqrt{5}}\right).

We'll set up the iterated integral using horizontal strips as in the sketch

Figure from prob_s3.2, line 1797

Figure from prob_s3.2, line 1797

Looking at that sketch, we see that, on GG,

  • yy runs from 00 to 25\frac{2}{\sqrt{5}}, and

  • for each fixed yy between 00 and 15\frac{1}{\sqrt{5}}, xx runs from y2\frac{y}{2} to 2y2y, and

  • for each fixed yy between 15\frac{1}{\sqrt{5}} and 25\frac{2}{\sqrt{5}} xx runs from y2\frac{y}{2} to 1y2\sqrt{1-y^2}.

So

Gf(x,y) dA=015dyy/22ydx f(x,y)+1525dyy/21y2dx f(x,y)\begin{align*} \dblInt_G f(x,y)\ \dee{A} &=\int_0^{\frac{1}{\sqrt{5}}}\dee{y}\int_{y/2}^{2y}\dee{x}\ f(x,y) +\int_{\frac{1}{\sqrt{5}}}^{\frac{2}{\sqrt{5}}}\dee{y}\int_{y/2}^{\sqrt{1-y^2}} \dee{x}\ f(x,y) \end{align*}

(b) In polar coordinates

  • the equation x2+y2=1x^2+y^2=1 becomes r=1r=1, and

  • the equation y=x/2y=x/2 becomes rsinθ=r2cosθr\sin\theta = \frac{r}{2}\cos\theta or tanθ=12\tan\theta =\frac{1}{2}, and

  • the equation y=2xy=2x becomes rsinθ=2rcosθr\sin\theta = 2r\cos\theta or tanθ=2\tan\theta =2.

Looking at the sketch

Figure from prob_s3.2, line 1797

Figure from prob_s3.2, line 1797

we see that, on GG,

  • θ\theta runs from arctan12\arctan\frac{1}{2} to arctan2\arctan 2, and

  • for each fixed θ\theta in that range, rr runs from 00 to 11.

As dA=rdrdθ\dee{A}=r\,\dee{r}\,\dee{\theta}, and x=rcosθx=r\cos\theta, y=rsinθy=r\sin\theta,

Gf(x,y) dA=arctan12arctan2dθ01dr rf(rcosθ,rsinθ)\begin{align*} \dblInt_G f(x,y)\ \dee{A} &=\int_{\arctan\frac{1}{2}}^{\arctan 2}\dee{\theta} \int_0^1\dee{r}\ r\,f(r\cos\theta,r\sin\theta) \end{align*}
Q21Stage 3Past exam · M200 2011A

Consider

J=02y4y2yxex2+y2 dxdy\begin{equation*} J = \int_0^{\sqrt{2}} \int_y^{\sqrt{4-y^2}} \frac{y}{x} e^{x^2+y^2}\ \dee{x}\,\dee{y} \end{equation*}
  1. Sketch the region of integration.

  2. Reverse the order of integration.

  3. Evaluate JJ by using polar coordinates.

Answer

(a)

Figure from prob_s3.2, line 1912

Figure from prob_s3.2, line 1912

(b) J=020xyxex2+y2 dydx+2204x2yxex2+y2 dydxJ = \int_0^{\sqrt{2}}\int_0^x \frac{y}{x} e^{x^2+y^2}\ \dee{y}\,\dee{x} + \int_{\sqrt{2}}^2\int_0^{\sqrt{4-x^2}} \frac{y}{x} e^{x^2+y^2}\ \dee{y}\,\dee{x}

(c) 14[e41]ln2\frac{1}{4}\left[e^4-1\right]\ln 2

Full solution

(a) On the domain of integration

  • yy runs from 00 to 2\sqrt{2} and

  • for each yy in that range, xx runs from yy to 4y2\sqrt{4-y^2}. We can rewrite x=4y2x=\sqrt{4-y^2} in the more familiar form x2+y2=4x^2+y^2=4, x0x\ge 0.

The figure on the left below provides a sketch of the domain of integration. It also shows the generic horizontal slice that was used to set up the given iterated integral.

Figure from prob_s3.2, line 1926

Figure from prob_s3.2, line 1926

Figure from prob_s3.2, line 1926

Figure from prob_s3.2, line 1926

(b) To reverse the order of integration observe, we use vertical, rather than horizontal slices. From the figure on the right above that, on the domain of integration,

  • xx runs from 00 to 22 and

  • for each xx in the range 0x20\le x\le\sqrt{2}, yy runs from 00 to xx.

  • for each xx in the range 2x2\sqrt{2}\le x\le 2, yy runs from 00 to 4x2\sqrt{4-x^2}.

So the integral

J=020xyxex2+y2 dydx+2204x2yxex2+y2 dydx\begin{equation*} J = \int_0^{\sqrt{2}}\int_0^x \frac{y}{x} e^{x^2+y^2}\ \dee{y}\,\dee{x} + \int_{\sqrt{2}}^2\int_0^{\sqrt{4-x^2}} \frac{y}{x} e^{x^2+y^2}\ \dee{y}\,\dee{x} \end{equation*}

(c) In polar coordinates, the line y=xy=x is θ=π4\theta=\frac{\pi}{4}, the circle x2+y2=4x^2+y^2=4 is r=2r=2, and dxdy=rdrdθ\dee{x}\,\dee{y}=r\,\dee{r}\,\dee{\theta}. So

J=0π/4dθ02dr rrsinθrcosθyxer2=0π/4dθ sinθcosθ[12er2]02=12[e41]11/2du 1uwith u=cosθ, du=sinθdθ=12[e41] [lnu]11/2=14[e41]ln2\begin{align*} J&=\int_0^{\pi/4}\dee{\theta}\int_0^2\dee{r}\ r \overbrace{\frac{r\sin\theta}{r\cos\theta}}^{\frac{y}{x}}e^{r^2} \\ &=\int_0^{\pi/4}\dee{\theta}\ \frac{\sin\theta}{\cos\theta} \left[\frac{1}{2} e^{r^2}\right]_0^2 \\ &=-\frac{1}{2}\left[e^4-1\right] \int_1^{1/\sqrt{2}}\dee{u}\ \frac{1}{u} \qquad\text{with }u=\cos\theta,\ \dee{u}=-\sin\theta\,\dee{\theta} \\ &=-\frac{1}{2}\left[e^4-1\right]\ \Big[\ln|u|\Big]_1^{1/\sqrt{2}} \\ &= \frac{1}{4}\left[e^4-1\right]\ln 2 \end{align*}
Q22Stage 3

Find the volume of the region in the first octant below the paraboloid

z=1x2a2y2b2z=1-\frac{x^2}{a^2}-\frac{y^2}{b^2}
Answer

π8ab\frac{\pi}{8}ab

Full solution

The paraboloid hits the xyxy–plane at x2a2+y2b2=1\frac{x^2}{a^2} +\frac{y^2}{b^2}=1.

Volume=0adx0b1x2a2dy (1x2a2y2b2)=b0adx01x2a2dv (1x2a2v2) where y=bv\begin{align*} \text{Volume} &=\int_0^a \dee{x}\int_0^{b\sqrt{1-{x^2\over a^2}}} \dee{y}\ \left(1-\frac{x^2}{a^2}-\frac{y^2}{b^2}\right) \cr &=b\int_0^a \dee{x}\int_0^{\sqrt{1-{x^2\over a^2}}} \dee{v}\ \left(1-\frac{x^2}{a^2}-v^2\right) \qquad\text{ where }y=bv\cr \end{align*}

Think of this integral as being of the form

b0adx g(x)withg(x)=01x2a2dv (1x2a2v2)\begin{equation*} \displaystyle b\int_0^a \dee{x}\ g(x)\quad \text{with}\quad \displaystyle g(x)=\int_0^{\sqrt{1-{x^2\over a^2}}} \dee{v}\ \left(1-\frac{x^2}{a^2}-v^2\right) \end{equation*}

Then, substituting x=aux=au,

Volume=ab01du01u2dv (1u2v2)=abu2+v21u,v0dudv (1u2v2)\begin{align*} \text{Volume} &=ab\int_0^1 \dee{u}\int_0^{\sqrt{1-u^2}} \dee{v}\ \big(1-u^2-v^2\big) \\ &=ab\dblInt_{u^2+v^2\le 1\atop u,v\ge 0} \dee{u} \dee{v}\ \big(1-u^2-v^2\big) \end{align*}

Now switch to polar coordinates using u=rcosθu=r\cos\theta, v=rsinθv=r\sin\theta.

Volume=ab01dr0π2dθ r(1r2)=ab π2 [r22r44]01=π8ab\begin{align*} \text{Volume} &=ab\int_0^1 \dee{r}\int_0^{\pi\over 2} \dee{\theta}\ r\big(1-r^2\big) =ab\ \frac{\pi}{2}\ \left[\frac{r^2}{2}-\frac{r^4}{4}\right]_0^1 =\frac{\pi}{8}ab \end{align*}
Q23Stage 3

A symmetrical coffee percolator holds 24 cups when full. The interior has a circular cross-section which tapers from a radius of 3" at the centre to 2" at the base and top, which are 12" apart. The bounding surface is parabolic. Where should the mark indicating the 6 cup level be placed?

Figure from prob_s3.2, line 2032

Figure from prob_s3.2, line 2032

Answer

About 3.5” above the bottom

Full solution

Let r(z)r(z) be the radius of the urn at height zz above its middle. Because the bounding surface of the urn is parabolic, r(z)r(z) must be a quadratic function of zz that varies between 33 at z=0z=0 and 22 at z=±6z=\pm 6. That is, r(z)r(z) must be of the form r(z)=az2+bz+cr(z)=az^2+bz+c. The condition that r(0)=3r(0)=3 tells us that c=3c=3. The conditions that r(±6)=2r(\pm 6)=2 tells us that

62a+6b+3=262a6b+3=2\begin{align*} 6^2a + 6b + 3 &=2 \\ 6^2a - 6b + 3 &=2 \end{align*}

So b=0b=0 and 62a=16^2a=-1 so that a=162a=-\frac{1}{6^2}. All together r(z)=3(z6)2r(z)=3-\big(\frac{z}{6}\big)^2.

Slice the urn into horzontal slices, with the slice at height zz a disk of radius r(z)r(z) and thickness dz\dee{z} and hence of volume πr(z)2dz\pi r(z)^2\dee{z}. The volume to height z0z_0 is

V(z)=6z0dz πr(z)2=6z0dz π[3z236]2=π[9zz318+z55×362]6z0\begin{align*} V(z) &=\int_{-6}^{z_0} \dee{z}\ \pi r(z)^2 =\int_{-6}^{z_0} \dee{z}\ \pi\left[3-\frac{z^2}{36}\right]^2 =\pi\left[9z-\frac{z^3}{18}+\frac{z^5}{5\times36^2}\right]_{-6}^{z_0}\cr \end{align*}

We are told that the mark is to be at the 6 cup level and that the urn holds 24 cups. So the mark is to be at the height z0z_0 for which the volume, V(z0)V(z_0), is one quarter of the total volume, V(6)V(6).
That is, we are to choose z0z_0 so that V(z0)=14V(6)V(z_0)=\frac{1}{4} V(6) or

π[9zz318+z55×362]6z0=π4[9zz318+z55×362]66=π2[9×66318+655×362]\begin{equation*} \pi\left[9z-\frac{z^3}{18}+\frac{z^5}{5\times36^2}\right]_{-6}^{z_0} =\frac{\pi}{4}\left[9z-\frac{z^3}{18}+\frac{z^5}{5\times36^2}\right]_{-6}^{6} =\frac{\pi}{2}\left[9\times 6-\frac{6^3}{18}+\frac{6^5}{5\times36^2}\right] \end{equation*}

or

9z0z0318+z055×362=12[9×66318+655×362]=21.60\begin{equation*} 9z_0-\frac{z_0^3}{18}+\frac{z_0^5}{5\times36^2} =-\frac{1}{2}\left[9\times 6-\frac{6^3}{18}+\frac{6^5}{5\times36^2}\right] =-21.60 \end{equation*}

Since [9z0z0318+z056480]z0=2.495=21.61\Big[9z_0-\frac{z_0^3}{18}+\frac{z_0^5}{6480}\Big]_{z_0=-2.495}=-21.61 and [9z0z0318+z056480]z0=2.490=21.57\Big[9z_0-\frac{z_0^3}{18}+\frac{z_0^5}{6480}\Big]_{z_0=-2.490}=-21.57, there is a solution z0=2.49z_0=-2.49 (to two decimal places). The mark should be about 3.5” above the bottom.

Q24Stage 3Past exam · M200 2003A

Consider the surface SS given by z=ex2+y2z=e^{x^2+y^2}.

  1. Compute the volume under SS and above the disk x2+y29x^2+y^2\le 9 in the xyxy-plane.

  2. The volume under SS and above a certain region RR in the xyxy-plane is

    01(0yex2+y2dx)dy+12(02yex2+y2dx)dy\begin{equation*} \int_0^1\bigg(\int_0^y e^{x^2+y^2}\,\dee{x}\bigg)\dee{y} +\int_1^2\bigg(\int_0^{2-y} e^{x^2+y^2}\,\dee{x}\bigg)\dee{y} \end{equation*}

    Sketch RR and express the volume as a single iterated integral with the order of integration reversed. Do not compute either integral in part (b).

Answer

(a) π(e91)25,453\pi\big(e^9-1\big)\approx 25,453

(b) 01dxx2xdy ex2+y2\int_0^1 \dee{x}\int_x^{2-x}\dee{y}\ e^{x^2+y^2}

Figure from prob_s3.2, line 2116

Figure from prob_s3.2, line 2116

Full solution

(a) In polar coordinates, the base region x2+y29x^2+y^2\le 9 is r3r\le 3, 0θ2π0\le\theta\le 2\pi. So the

Volume=x2+y29ex2+y2 dxdy=03dr02πdθ rer2=2π03dr rer2=πer203=π(e91)25,453\begin{align*} \text{Volume} &=\dblInt_{x^2+y^2\le 9} e^{x^2+y^2}\ \dee{x}\dee{y} =\int_0^3 \dee{r}\int_0^{2\pi}\dee{\theta}\ r e^{r^2} =2\pi\int_0^3\dee{r}\ r e^{r^2} =\pi e^{r^2}\Big|_0^3 \\ &=\pi\big(e^9-1\big)\approx 25,453 \end{align*}

(b) The two integrals have domains

{ (x,y)  0y1, 0xy }{ (x,y)  1y2, 0x2y }\begin{align*} \Set{(x,y)}{0\le y\le 1,\ 0\le x\le y}\qquad \Set{(x,y)}{1\le y\le 2,\ 0\le x\le 2-y} \end{align*}

The union of those two domains (as well as horizontal strips that were used in setting up the two given integrals) is sketched in the figure on the left below.

Figure from prob_s3.2, line 2125

Figure from prob_s3.2, line 2125

Figure from prob_s3.2, line 2125

Figure from prob_s3.2, line 2125

To reverse the order of integration, we decompose the domain using vertical strips as in the figure on the right above. As

  • xx runs from 00 to 11 and

  • for each fixed xx between 00 and 11, yy runs from xx to 2x2-x.

we have that the

Volume=01dxx2xdy ex2+y2\begin{equation*} \text{Volume}=\int_0^1 \dee{x}\int_x^{2-x}\dee{y}\ e^{x^2+y^2} \end{equation*}

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From the UBC Math 200 open textbook project, © Joel Feldman, Andrew Rechnitzer, Elyse Yeager and others. Licensed CC BY-NC-SA 4.0; this HTML adaptation is released under the same licence. Full attribution.