These Further Maths polar coordinates worksheet answers give a full worked solution to all 20 questions of the polar coordinates worksheet. Try each question yourself first, then check your method step by step.
Answer to Question 1
Method: use \(x=r\cos\theta\), \(y=r\sin\theta\) to go from polar to Cartesian, and \(r=\sqrt{x^2+y^2}\), \(\tan\theta=\dfrac yx\) to go back. Always plot the point to choose the correct quadrant for \(\theta\).
- \(x=4\cos\tfrac\pi3=4\times\tfrac12=2\) and \(y=4\sin\tfrac\pi3=4\times\tfrac{\sqrt3}2=2\sqrt3\): \((2,2\sqrt3)\) This point is in the first quadrant, as expected for \(\theta=\tfrac\pi3\).
- \(x=2\sqrt2\cos\tfrac{3\pi}4=2\sqrt2\times(-\tfrac{\sqrt2}2)=-2\) and \(y=2\sqrt2\times\tfrac{\sqrt2}2=2\): \((-2,2)\) This point is in the second quadrant.
- \(r=\sqrt{9+27}=\sqrt{36}=6\). The point is in the second quadrant, so \(\theta=\pi-\arctan\dfrac{3\sqrt3}3=\pi-\tfrac\pi3=\tfrac{2\pi}3\): \((6,\tfrac{2\pi}3)\) Check: \(6\cos\tfrac{2\pi}3=-3\) and \(6\sin\tfrac{2\pi}3=3\sqrt3\).
- \(r=\sqrt{25+144}=13\). The point is in the fourth quadrant, so \(\theta=-\arctan\tfrac{12}5=-1.176\): \((13,\,-1.176)\) A calculator gives \(\arctan\tfrac{-12}5\) directly in the fourth quadrant here.
Answer to Question 2
- Multiply by \(r\): \(r^2=4r\cos\theta\), so \(x^2+y^2=4x\), i.e. \((x-2)^2+y^2=4\): a circle with centre \((2,0)\) and radius 2.
- \(r\cos\theta=2\), so \(x=2\): a vertical straight line.
- \(\sin2\theta=2\sin\theta\cos\theta\), so \(2(r\sin\theta)(r\cos\theta)=8\), i.e. \(2xy=8\): \(xy=4\), a rectangular hyperbola.
- \(r-r\cos\theta=2\), so \(r=x+2\). Square: \(x^2+y^2=x^2+4x+4\), so \(y^2=4x+4\), a parabola with vertex \((-1,0)\).
Answer to Question 3
Method: replace \(x^2+y^2\) by \(r^2\), \(x\) by \(r\cos\theta\) and \(y\) by \(r\sin\theta\), then divide by any common power of \(r\) (the pole is usually still on the curve).
- \(r^2=9\), so \(r=3\): a circle centred at the pole.
- \(\tan\theta=1\) with \(x>0\): \(\theta=\tfrac\pi4\), a half-line from the pole.
- \(r^2=6r\sin\theta\), so \(r=6\sin\theta\) (a circle through the pole with centre \((0,3)\)).
- \(r^4=4r^2\sin\theta\cos\theta=2r^2\sin2\theta\), so \(r^2=2\sin2\theta\).
Answer to Question 4
- \(r=4,\;3,\;2,\;1,\;0\)
- \(\cos(-\theta)=\cos\theta\), so the points \((r,\theta)\) and \((r,-\theta)\) are both on the curve: the curve is its own reflection in the initial line.
- \(\cos\theta\le1\), so \(r_{\max}=4\) at \(\theta=0\); \(r=0\) when \(\cos\theta=-1\), i.e. \(\theta=\pi\).
- The curve is a cardioid (heart shape) with its cusp at the pole:
Answer to Question 5
Method: the area swept out by a polar curve is \(A=\tfrac12\displaystyle\int_\alpha^\beta r^2\,d\theta\). Square \(r\) first, replace \(\cos^2\theta\) or \(\sin^2\theta\) by double angle expressions, then integrate term by term.
- Here \(r^2=9\) is constant and a full turn is \(0\le\theta\le2\pi\). \(A=\tfrac12\displaystyle\int_0^{2\pi}9\,d\theta=\tfrac12\times9\times2\pi=\) \(9\pi\) \(=\pi\times3^2\) β The formula agrees with \(\pi r^2\).
- The cardioid is traced once as \(\theta\) goes from 0 to \(2\pi\). Use \(\cos^2\theta=\tfrac12(1+\cos2\theta)\). \(r^2=4(1+2\cos\theta+\cos^2\theta)=4\left(\tfrac32+2\cos\theta+\tfrac12\cos2\theta\right)\). Integrating from 0 to \(2\pi\) the cosine terms give 0, so \(A=\tfrac12\times4\times\tfrac32\times2\pi=\) \(6\pi\). So the cardioid encloses \(6\pi\approx18.8\) square units.
- The spiral and the initial line enclose the region swept as \(\theta\) goes from 0 to \(\pi\). \(A=\tfrac12\displaystyle\int_0^\pi\theta^2\,d\theta=\tfrac12\left[\tfrac{\theta^3}3\right]_0^\pi=\) \(\dfrac{\pi^3}6\) \(\approx5.17\) So the area is \(\tfrac{\pi^3}6\).
Answer to Question 6
- \(r\sin\theta=\sin\theta+\sin\theta\cos\theta=\sin\theta+\tfrac12\sin2\theta\). Differentiate: \(\cos\theta+\cos2\theta=\cos\theta+2\cos^2\theta-1\) β
- \(2\cos^2\theta+\cos\theta-1=(2\cos\theta-1)(\cos\theta+1)=0\), so \(\cos\theta=\tfrac12\) (or \(\cos\theta=-1\), which is the pole). \(\theta=\pm\tfrac\pi3\) and \(r=\tfrac32\): \((\tfrac32,\tfrac\pi3)\) and \((\tfrac32,-\tfrac\pi3)\).
- \(r\cos\theta=\cos\theta+\cos^2\theta\), derivative \(-\sin\theta-2\sin\theta\cos\theta=-\sin\theta(1+2\cos\theta)=0\). \(\sin\theta=0\): \(\theta=0\), \(r=2\). \(\cos\theta=-\tfrac12\): \(\theta=\pm\tfrac{2\pi}3\), \(r=\tfrac12\). \((2,0)\), \((\tfrac12,\tfrac{2\pi}3)\) and \((\tfrac12,-\tfrac{2\pi}3)\) (\(\theta=\pi\) gives the pole, where the curve has a cusp).
Answer to Question 7
- \(P\): \((40\cos\tfrac\pi6,\;40\sin\tfrac\pi6)=\) \((34.64,\;20)\). \(Q\): \((30\cos\tfrac{2\pi}3,\;30\sin\tfrac{2\pi}3)=\) \((-15,\;25.98)\).
- \(\tfrac{2\pi}3-\tfrac\pi6=\) \(\tfrac\pi2\), a right angle.
- By the cosine rule, \(PQ^2=40^2+30^2-2\times40\times30\cos\tfrac\pi2=1600+900-0=2500\), so \(PQ=50\) km (or use Pythagoras since the angle is \(90^\circ\)).
- The aircraft are 50 km apart, well above 5 km, so they are safely separated at the moment.
Answer to Question 8
- \(\cos\theta\) ranges from \(-1\) to \(1\), so greatest 6 m (at \(\theta=0\)) and least 2 m (at \(\theta=\pi\)).
- \(A=\tfrac12\displaystyle\int_0^{2\pi}(16+16\cos\theta+4\cos^2\theta)\,d\theta\). With \(4\cos^2\theta=2+2\cos2\theta\): \(A=\tfrac12\displaystyle\int_0^{2\pi}(18+16\cos\theta+2\cos2\theta)\,d\theta=\tfrac12\times18\times2\pi=\) \(18\pi\) β (about 56.5 mΒ²).
- \(\dfrac{18\pi}{80}\times100=\) 70.7%
- \(r=4+2\cos\theta\ge4-2=2>0\) for every \(\theta\), so \(r\) is never zero.
Answer to Question 9
- \(r=\tfrac\pi4,\;\tfrac\pi2,\;\pi,\;2\pi\)
- Along the initial line the spiral crosses at \(\theta=2\pi,4\pi,\dots\), where \(r=\pi,2\pi,\dots\). The gap is \(\pi\) dm \(\approx3.14\) dm.
- \(A=\tfrac12\displaystyle\int_0^{2\pi}\tfrac14\theta^2\,d\theta=\tfrac18\left[\tfrac{\theta^3}3\right]_0^{2\pi}=\dfrac{8\pi^3}{24}=\dfrac{\pi^3}3\approx\) 10.3 dmΒ².
- The gap between turns is \(\pi\) dm \(\approx31.4\) cm, which is much more than the 3 cm width, so the turns do not touch. For \(r=k\theta\) the gap is \(2\pi k\) dm. Setting \(2\pi k=0.3\) dm gives \(k=\dfrac{0.3}{2\pi}\approx0.0477\) dm per radian.
Answer to Question 10
- \(\sin2\theta\ge0\) for \(0\le\theta\le\tfrac\pi2\), starting and ending at \(r=0\): one petal. The greatest value \(r=3\) occurs at \(\theta=\tfrac\pi4\), so each petal is 3 cm long.
- \(A=\tfrac12\displaystyle\int_0^{\pi/2}9\sin^22\theta\,d\theta=\tfrac94\displaystyle\int_0^{\pi/2}(1-\cos4\theta)\,d\theta=\tfrac94\times\tfrac\pi2=\) \(\dfrac{9\pi}8\) cmΒ² \(\approx3.53\) cmΒ²
- \(4\times\dfrac{9\pi}8=\) \(\dfrac{9\pi}2\approx14.1\) cmΒ²
- \(14.137\times2=28.3\)p, so about 28p.
Answer to Question 11
Method: the area swept out by a polar curve is \(A=\tfrac12\displaystyle\int_\alpha^\beta r^2\,d\theta\). Square \(r\) first, replace \(\cos^2\theta\) or \(\sin^2\theta\) by double angle expressions, then integrate term by term.
- Solve the equation \(1+\cos\theta=1.5\) for \(-180^\circ\lt \theta\le180^\circ\). \(1+\cos\theta=1.5\) gives \(\cos\theta=0.5\): \(\theta=\pm60^\circ\). So the sensitivity is 1.5 at \(60^\circ\) either side of the singer.
- Expand \(r^2\) and use \(\int_0^{2\pi}\cos^2\theta\,d\theta=\pi\). \(A=\tfrac12\displaystyle\int_0^{2\pi}(1+2\cos\theta+\cos^2\theta)\,d\theta=\tfrac12(2\pi+0+\pi)=\) \(\dfrac{3\pi}2\) So the whole curve encloses \(\tfrac{3\pi}2\approx4.71\) square units.
- \(\tfrac12\displaystyle\int_{-\pi/2}^{\pi/2}\left(\tfrac32+2\cos\theta+\tfrac12\cos2\theta\right)d\theta=\tfrac12\left[\tfrac32\theta+2\sin\theta+\tfrac14\sin2\theta\right]_{-\pi/2}^{\pi/2}=\tfrac12\left(\tfrac{3\pi}2+4+0\right)=\dfrac{3\pi}4+2\) β This is the required result, about 4.36.
- \(\dfrac{3\pi/4+2}{3\pi/2}=\dfrac12+\dfrac4{3\pi}=0.924\), so about 92% lies in front: the microphone mostly ignores sound from the speakers behind it, which reduces feedback.
Answer to Question 12
- \(\theta=0\): \(r=8\); \(\theta=\pi\): \(r=2\), on the other side of the hut. Total \(8+2=\) 10, i.e. 1000 m.
- \(A=\tfrac12\displaystyle\int_0^{2\pi}(25+30\cos\theta+9\cos^2\theta)\,d\theta=\tfrac12(50\pi+0+9\pi)=\dfrac{59\pi}2\approx92.7\) (hundreds of m)Β². Each unit is \(100\times100=10\,000\) mΒ², so the area is about 927 000 mΒ².
- \(a=5\), \(2b=6\), and \(5<6\), so the course is not convex: it has a slight dent (dimple) near \(\theta=\pi\), where the runner turns slightly the other way.
Answer to Question 13
- The coast is the line \(x=4\), i.e. \(r\cos\theta=4\), so \(r=\dfrac4{\cos\theta}=4\sec\theta\) β
- \(r=4\sec\tfrac\pi3=4\times2=\) 8 km; the point is \((8\cos\tfrac\pi3,\;8\sin\tfrac\pi3)=\) \((4,\;4\sqrt3)\).
- \(A=\tfrac12\displaystyle\int_0^{\pi/3}16\sec^2\theta\,d\theta=8\left[\tan\theta\right]_0^{\pi/3}=\) \(8\sqrt3\approx13.9\) kmΒ²
- The region is a right-angled triangle with vertices \((0,0)\), \((4,0)\) and \((4,4\sqrt3)\): area \(\tfrac12\times4\times4\sqrt3=8\sqrt3\) β
Answer to Question 14
- \(r\) is least when \(\cos\theta=1\): \(r=\dfrac{8000}{1.2}=\) 6667 km (perigee). \(r\) is greatest when \(\cos\theta=-1\): \(r=\dfrac{8000}{0.8}=\) 10 000 km (apogee).
- \(\cos\tfrac\pi2=0\), so \(r=8000\) km.
- \(6667-6370=\) about 297 km.
- \(\cos(-\theta)=\cos\theta\), so \((r,\theta)\) and \((r,-\theta)\) both lie on the orbit: reflection in the initial line maps the orbit to itself.
Answer to Question 15
- \(3\cos\theta=1+\cos\theta\) gives \(\cos\theta=\tfrac12\), so \(\theta=\pm\tfrac\pi3\) and \(r=\tfrac32\): \((\tfrac32,\tfrac\pi3)\) and \((\tfrac32,-\tfrac\pi3)\).
- \(C_1\) passes through the pole at \(\theta=\pm\tfrac\pi2\) and \(C_2\) at \(\theta=\pi\). Equating \(r\)-values only finds intersections at the same \(\theta\), so the pole must be checked separately.
- \(R\) is the crescent between the two intersection points, for \(-\tfrac\pi3\le\theta\le\tfrac\pi3\), where the circle is outside the cardioid.
- By symmetry \(A=2\times\tfrac12\displaystyle\int_0^{\pi/3}\left(9\cos^2\theta-(1+\cos\theta)^2\right)d\theta=\displaystyle\int_0^{\pi/3}(8\cos^2\theta-2\cos\theta-1)\,d\theta\). With \(8\cos^2\theta=4+4\cos2\theta\): \(\displaystyle\int_0^{\pi/3}(3+4\cos2\theta-2\cos\theta)\,d\theta=\left[3\theta+2\sin2\theta-2\sin\theta\right]_0^{\pi/3}=\pi+\sqrt3-\sqrt3=\) \(\pi\) β
- \(r^2=3r\cos\theta\) gives \(x^2+y^2=3x\), i.e. \((x-\tfrac32)^2+y^2=\tfrac94\): radius \(\tfrac32\), area \(\tfrac94\pi\). Check: \(\tfrac12\displaystyle\int_{-\pi/2}^{\pi/2}9\cos^2\theta\,d\theta=\tfrac92\times\tfrac\pi2=\tfrac{9\pi}4\) β
Answer to Question 16
- \(r\sin\theta=3\sin\theta+\sin2\theta\), so the derivative is \(3\cos\theta+2\cos2\theta=3\cos\theta+4\cos^2\theta-2\) β
- \(\cos\theta=\dfrac{-3+\sqrt{9+32}}8=\dfrac{-3+\sqrt{41}}8=0.4254\) (the other root is less than \(-1\)). \(\theta=1.131\). Then \(r=3+2(0.4254)=3.851\) and the tangent is \(y=r\sin\theta=3.851\times0.9050=\) 3.485 units from the initial line.
- \(r\cos\theta=3\cos\theta+2\cos^2\theta\), derivative \(-3\sin\theta-4\sin\theta\cos\theta=-\sin\theta(3+4\cos\theta)\) β
- \(\sin\theta=0\): \(\theta=0\) (\(r=5\)) and \(\theta=\pi\) (\(r=1\)). \(\cos\theta=-\tfrac34\): \(\theta=\pm2.419\), \(r=3-\tfrac32=1.5\) and \(x=1.5\times(-\tfrac34)=\) \(-1.125\). Points: \((5,0)\), \((1,\pi)\), \((1.5,\pm2.419)\).
- At \(\theta=\pi\) the curve is at \(x=-1\), but at \(\theta=\pm2.419\) it reaches further left, \(x=-1.125\). So the leftmost part of the curve bends inwards at \(\theta=\pi\): a dimple (this agrees with \(a=3<2b=4\)).
Answer to Question 17
- \(\cos2\theta\ge0\) when \(-\tfrac\pi4\le\theta\le\tfrac\pi4\) or \(\tfrac{3\pi}4\le\theta\le\pi\), \(-\pi\lt \theta\le-\tfrac{3\pi}4\). \(r_{\max}=2\) at \(\theta=0\) and \(\theta=\pi\).
- One loop: \(\tfrac12\displaystyle\int_{-\pi/4}^{\pi/4}4\cos2\theta\,d\theta=\left[\sin2\theta\right]_{-\pi/4}^{\pi/4}=1-(-1)=\) 2. Total area 4.
- \(y=r\sin\theta\), so \(y^2=r^2\sin^2\theta=4\cos2\theta\sin^2\theta\) β. Product rule: \(-2\sin2\theta\sin^2\theta+\cos2\theta\cdot2\sin\theta\cos\theta=\sin2\theta(\cos2\theta-2\sin^2\theta)=\sin2\theta(\cos2\theta-(1-\cos2\theta))=\sin2\theta(2\cos2\theta-1)\) β
- The maximum of \(y\) in \((0,\tfrac\pi4)\) needs \(\cos2\theta=\tfrac12\), so \(\theta=\tfrac\pi6\) and \(r^2=2\), \(r=\sqrt2\). Height \(y=\sqrt2\sin\tfrac\pi6=\dfrac{\sqrt2}2\approx0.707\).
- \(r^2=4(\cos^2\theta-\sin^2\theta)\). Multiply by \(r^2\): \(r^4=4(r^2\cos^2\theta-r^2\sin^2\theta)\), so \((x^2+y^2)^2=4(x^2-y^2)\) β
Answer to Question 18
- \(r=2\pi\) and \(r=4\pi\)
- \(\tfrac12\displaystyle\int_0^{2\pi}\theta^2\,d\theta=\tfrac16(2\pi)^3=\) \(\dfrac{4\pi^3}3\)
- \(\tfrac12\displaystyle\int_{2\pi}^{4\pi}\theta^2\,d\theta=\tfrac16(64\pi^3-8\pi^3)=\) \(\dfrac{28\pi^3}3\)
- The second sweep covers the region inside the second turn, which includes the region inside the first turn; removing that leaves the strip. \(\dfrac{28\pi^3}3-\dfrac{4\pi^3}3=\) \(8\pi^3\approx248\) mmΒ² β
- The sweep for turn \(n+1\) is \(\tfrac16\left((2n+2)^3-(2n)^3\right)\pi^3\) and for turn \(n\) is \(\tfrac16\left((2n)^3-(2n-2)^3\right)\pi^3\). Their difference is \(\tfrac{8\pi^3}6\left((n+1)^3-2n^3+(n-1)^3\right)=\tfrac{8\pi^3}6\times6n=\) \(8n\pi^3\), which increases by \(8\pi^3\) each time: an arithmetic sequence.
Answer to Question 19
- \(r=0,\;\sqrt2,\;2,\;\sqrt2,\;0\). \(r\) starts and ends at 0 and is positive in between: one petal, centred on \(\theta=0\).
- \(r=2\) when \(\cos3\theta=1\): \(3\theta=0,\pm2\pi\), so \(\theta=0\), \(\pm\tfrac{2\pi}3\).
- \(\tfrac12\displaystyle\int_{-\pi/6}^{\pi/6}4\cos^23\theta\,d\theta=\displaystyle\int_{-\pi/6}^{\pi/6}(1+\cos6\theta)\,d\theta=\tfrac\pi3+0=\) \(\dfrac\pi3\). Total \(\pi\).
- \(\dfrac{\pi}{4\pi}=\) \(\dfrac14\)
- The area of a petal is proportional to \(a^2\): \(\dfrac{a^2}4\times\dfrac\pi3=3\), so \(a^2=\dfrac{36}\pi\) and \(a=\dfrac6{\sqrt\pi}\approx3.39\) cm.
Answer to Question 20
- \(A=\tfrac12a^2\displaystyle\int_0^{2\pi}\left(\tfrac32+2\cos\theta+\tfrac12\cos2\theta\right)d\theta=\tfrac12a^2\times3\pi=\tfrac32\pi a^2\). The circle \(r=a\) has area \(\pi a^2\), so the ratio is \(\tfrac32\) β
- \(r=a+a\cos\theta\); multiply by \(r\): \(r^2=ar+ax\), so \(r^2-ax=ar\). Square: \((x^2+y^2-ax)^2=a^2r^2=\) \(a^2(x^2+y^2)\) β
- \(y=a(1+\cos\theta)\sin\theta\), \(\dfrac{dy}{d\theta}=a(\cos\theta+\cos2\theta)=a(2\cos\theta-1)(\cos\theta+1)=0\) gives \(\theta=\tfrac\pi3\) and \(y=a\cdot\tfrac32\cdot\tfrac{\sqrt3}2=\) \(\dfrac{3\sqrt3}4a\).
- The curves meet where \(\cos\theta=0\), \(\theta=\pm\tfrac\pi2\). For \(|\theta|\lt \tfrac\pi2\) the cardioid is outside the circle. Area \(=2\times\tfrac12\displaystyle\int_0^{\pi/2}a^2\left((1+\cos\theta)^2-1\right)d\theta=a^2\displaystyle\int_0^{\pi/2}\left(2\cos\theta+\tfrac12+\tfrac12\cos2\theta\right)d\theta=a^2\left(2+\tfrac\pi4\right)\): \(\left(2+\dfrac\pi4\right)a^2\).
How to use these Further Maths polar coordinates worksheet answers
First, try every question on the worksheet without looking. Then compare your working with the solution line by line, not only the final answer. When your answer is different, find the first step that changes, because that is where the mistake is. After that, read the matching part of the polar coordinates lesson again. Finally, check that the method is secure with the quiz or the test.
Also, the Further Maths polar coordinates worksheet answers are available as a PDF, so you can mark printed work quickly. Moreover, all the pages of this chapter work together, so you can move between them at any time. For example, many pupils read the lesson on Monday, practise on Wednesday and test themselves on Friday. In short, these Further Maths polar coordinates worksheet answers show every step, so nothing is left unexplained.


















