State the condition for a tangent at the pole
The tangents at the pole are the half-lines on which r vanishes.
Solve r=0
cos2θ=0 The zeros of the cosine give every direction in which the curve meets the pole.
List the solutions in the interval
θ=4π, θ=43π, θ=45π, θ=47π These are all the solutions with 0≤θ<2π.
Reject the stationary values of r
dθdr=0 gives the tips of the petals The tips are where r is greatest, not where it is zero.
Check one of the values
r(4π)=0 This confirms that the half-line really is a tangent at the pole.
Count the tangents
4 half-lines Each solution of r=0 contributes one tangent at the pole.
Recall the conversion formulae
x=rcosθ,y=rsinθ These take a point from polar form to Cartesian form.
Recall the reverse conversion formulae
r2=x2+y2,tanθ=xy These take a point from Cartesian form back to polar form.
Recall the polar area formula
A=21∫αβr2dθ The area is swept out by the radius vector between the two half-lines.
Recall the double-angle form of cos2θ
cos2θ=21(1+cos2θ) A squared cosine must be reduced to a multiple angle before it can be integrated.
Recall the double-angle form of sin2θ
sin2θ=21(1−cos2θ) A squared sine must be reduced to a multiple angle before it can be integrated.
Recall the condition for a tangent parallel to the initial line
dθdy=0wherey=rsinθ A horizontal tangent means y is stationary as θ varies.
Recall the condition for a tangent perpendicular to the initial line
dθdx=0wherex=rcosθ A vertical tangent means x is stationary as θ varies.
Recall the condition for a tangent at the pole
r=0 ⇒ θ=α is a tangent at the pole The curve reaches the pole along the half-line whose angle makes r vanish.
Recall the principal range for the polar angle
−π<θ≤π Every polar angle in this bank is given in the principal range.
Select the correct set of tangents
θ=4π, θ=43π, θ=45π, θ=47π These half-lines are exactly the tangents to C at the pole.