Finding vertical tangents to a limaçon

Let us find the vertical tangents to the limaçon (the cardioid) given by r=1+sin⁡θ.

Solution

(1) Convert to Cartesian parametric using x=rcos⁡θ and y=rsin⁡θ:

r(θ)=1+sin⁡θ≫≫(x,y)=((1+sin⁡θ)cos⁡θ,(1+sin⁡θ)sin⁡θ)

(2) Compute x′ and y′:

(x′(θ),y′(θ))≫≫(cos⁡θcos⁡θ+(1+sin⁡θ)(−sin⁡θ),cos⁡θsin⁡θ+(1+sin⁡θ)cos⁡θ)≫≫(cos2⁡θ−sin2⁡θ−sin⁡θ,cos⁡θ(1+2sin⁡θ))

(3) The vertical tangents occur when x′(θ)=0. We must double check that y′(θ)≠0 at these points.

x′(θ)=0≫≫cos2⁡θ−sin2⁡θ−sin⁡θ=0≫≫(1−sin2⁡θ)−sin2⁡θ−sin⁡θ=0

Substitute A=sin⁡θ and observe quadratic:

≫≫1−2A2−A=0≫≫2A2+A−1=0

Solve:

A=−b±b2−4ac2a≫≫−1±1−4⋅2⋅(−1)2⋅2≫≫12,−1

Then find θ:

A=sin⁡θ≫≫sin⁡θ=12,−1≫≫θ=π6,5π6(for 1/2)andθ=3π2(for −1)

(4) Compute the points. In polar coordinates:

(r,θ)=(1+sin⁡θ,θ)|θ=π6,5π6,3π2≫≫(32,π6),(32,5π6),(0,3π2)

In Cartesian coordinates:

At θ=π6:

(x,y)|θ=π6≫≫((1+sin⁡θ)cos⁡θ,(1+sin⁡θ)sin⁡θ)|θ=π6≫≫((1+12)32,(1+12)12)≫≫(334,34)

At θ=5π6:

(x,y)|θ=5π6≫≫((1+sin⁡θ)cos⁡θ,(1+sin⁡θ)sin⁡θ)|θ=5π6≫≫((1+12)−32,(1+12)12)≫≫(−334,34)

At θ=3π2:

(x,y)|θ=3π2≫≫((1+sin⁡θ)cos⁡θ,(1+sin⁡θ)sin⁡θ)|θ=3π2≫≫((1−1)⋅0,(1−1)⋅(−1))≫≫(0,0)

(5) Correction: (0,0) is a cusp!

The point (0,0) at θ=3π2 is on the cardioid, but the curve is not smooth there, this is a cusp.

Still, the left- and right-sided tangents exists and are equal, so in a certain sense we could say the curve has vertical tangent at θ=3π2.

Length of the inner loop

Consider the limaçon given by r(θ)=12+cos⁡θ.

How long is the inner loop? Set up an integral for this quantity.

Solution

The inner loop is traced by the moving point when 2π3≤θ≤4π3. This can be seen from the graph:

center

Therefore the length of the inner loop is given by this integral:

L=∫2π/34π/3(−sin⁡θ)2+(12+cos⁡θ)2dθ≫≫∫2π/34π/35/4+cos⁡θdθ

Area between circle and limaçon

Find the area of the region enclosed between the circle r0(θ)=1 and the limaçon r1(θ)=1+cos⁡θ.

Solution

First draw the region:

center

The two curves intersect at θ=±π2. Therefore the area enclosed is given by integrating over −π2≤θ≤+π2:

A=∫αβ12(r12−r02)dθ≫≫∫−π/2π/212((1+cos⁡θ)2−12)dθ≫≫12∫−π/2π/22cos⁡θ+cos2⁡θdθ≫≫∫−π/2π/2cos⁡θ+14(1+cos⁡(2θ))dθ≫≫sin⁡θ+θ4+18sin⁡(2θ)|−π/2π/2≫≫2+π4

Area of small loops

Consider the following polar graph of r(θ)=1+2cos⁡(4θ):

center

Find the area of the shaded region.

Solution

Find bounds for one small loop. Lower left loop occurs first. This loop is when 1+2cos⁡(4θ)≤0.

1+2cos⁡(4θ)≤0≫≫cos⁡(4θ)≤−12≫≫2π3≤4θ≤4π3≫≫π6≤θ≤π3

Now set up area integral:

A=4∫αβ12r(θ)2dθ≫≫4∫π/6π/312(1+2cos⁡(4θ))2dθ≫≫2∫π/6π/31+4cos⁡(4θ)+4cos2⁡(4θ)dθ

Power-to-frequency conversion: cos2⁡A⇝12(1+cos⁡(2A)) with A=4θ:

≫≫2∫π/6π/31+4cos⁡(4θ)+4⋅12(1+cos⁡(8θ))dθ≫≫6θ+2sin⁡(4θ)+14sin⁡(8θ)|π/6π/3≫≫π−332

Overlap area of circles

Compute the area of the overlap between crossing circles. For concreteness, suppose one of the circles is given by r(θ)=sin⁡θ and the other is given by r(θ)=cos⁡θ.

Solution

Drawing of the overlap:

center

Notice: total overlap area = 2× area of red region. Bounds for red region: 0≤θ≤π4.

Area formula applied to r(θ)=sin⁡θ:

A=2∫αβ12r(θ)2dθ≫≫2∫0π/412sin2⁡θdθ

Power-to-frequency: sin2⁡θ⇝12(1−cos⁡(2θ)):

≫≫2∫0π/414(1−cos⁡(2θ))dθ≫≫24θ−28sin⁡(2θ)|0π/4≫≫π8−14