These Further Maths further vectors worksheet answers give a full worked solution to all 20 questions of the further vectors worksheet. Try each question yourself first, then check your method step by step.
Answer to Question 1
Method: the scalar product is \(\mathbf a\cdot\mathbf b=a_1b_1+a_2b_2+a_3b_3=|\mathbf a||\mathbf b|\cos\theta\). Two non-zero vectors are perpendicular exactly when their scalar product is 0.
- Multiply corresponding components and add; use Pythagoras for the magnitudes. \(\mathbf a\cdot\mathbf b=2-4-6=\) \(-8\); \(|\mathbf a|=\sqrt{4+1+9}=\) \(\sqrt{14}\); \(|\mathbf b|=\sqrt{1+16+4}=\) \(\sqrt{21}\)
- Rearrange the scalar product formula for \(\cos\theta\). \(\cos\theta=\dfrac{-8}{\sqrt{14}\sqrt{21}}=\dfrac{-8}{\sqrt{294}}=-0.4666\), so \(\theta=\) 117.8\(^\circ\) The angle is obtuse because the scalar product is negative.
- Compute the scalar product. \(3-1-2=0\), so the vectors are perpendicular. So the two vectors are at \(90^\circ\).
- Set the scalar product equal to zero and solve for \(k\). \(3k+2k-4=0\), so \(k=\dfrac45\) Check: \(\tfrac{12}5+\tfrac85-4=0\).
Answer to Question 2
- \(\mathbf a\times\mathbf b=\begin{vmatrix}\mathbf i&\mathbf j&\mathbf k\\2&-1&3\\1&4&-2\end{vmatrix}=\mathbf i(2-12)-\mathbf j(-4-3)+\mathbf k(8+1)=\) \(-10\mathbf i+7\mathbf j+9\mathbf k\)
- \(\mathbf a\cdot(\mathbf a\times\mathbf b)=-20-7+27=0\) and \(\mathbf b\cdot(\mathbf a\times\mathbf b)=-10+28-18=0\). β
- Parallelogram: \(|\mathbf a\times\mathbf b|=\sqrt{100+49+81}=\sqrt{230}\approx\) 15.2. Triangle: half of this, 7.58.
Answer to Question 3
- \(\mathbf r=\begin{pmatrix}1\\2\\-1\end{pmatrix}+\lambda\begin{pmatrix}2\\-1\\3\end{pmatrix}\)
- \(\dfrac{x-1}2=\dfrac{y-2}{-1}=\dfrac{z+1}3\)
- Direction \(\overrightarrow{PQ}=\begin{pmatrix}2\\-2\\3\end{pmatrix}\), so \(\mathbf r=\begin{pmatrix}3\\0\\1\end{pmatrix}+\mu\begin{pmatrix}2\\-2\\3\end{pmatrix}\)
- For \((7,-4,7)\): \(3+2\mu=7\) gives \(\mu=2\); then \(y=-4\) β and \(z=1+6=7\) β. For \((1,2,-1)\): \(3+2\mu=1\) gives \(\mu=-1\), but then \(y=2\) β and \(z=1-3=-2\ne-1\), so it does not lie on the line.
Answer to Question 4
- \(\mathbf r\cdot\mathbf n=\mathbf a\cdot\mathbf n=2+6=8\), so \(2x-y+3z=8\). For \((3,1,1)\): \(6-1+3=8\) β.
- \(\overrightarrow{AB}=(-1,2,0)\) and \(\overrightarrow{AC}=(-1,0,3)\). Normal \(=\overrightarrow{AB}\times\overrightarrow{AC}=(6,3,2)\). Then \(6x+3y+2z=6\times1=6\): \(6x+3y+2z=6\). (Check \(B\): \(6\) β, \(C\): \(6\) β.)
- \(\mathbf r\cdot\begin{pmatrix}2\\-1\\3\end{pmatrix}=8\)
Answer to Question 5
Method: the angle between a line with direction \(\mathbf d\) and a plane with normal \(\mathbf n\) satisfies \(\sin\varphi=\dfrac{|\mathbf d\cdot\mathbf n|}{|\mathbf d||\mathbf n|}\) (the complement of the angle with the normal). The angle between two planes is the angle between their normals.
- Here \(\mathbf d=(1,2,2)\), \(\mathbf n=(2,-1,2)\) and both have magnitude 3. \(\sin\varphi=\dfrac{|\mathbf d\cdot\mathbf n|}{|\mathbf d||\mathbf n|}=\dfrac{|2-2+4|}{3\times3}=\dfrac49\), so \(\varphi=\) 26.4\(^\circ\) So the line meets the plane at about \(26.4^\circ\).
- The normals are \((1,2,2)\) with magnitude 3 and \((3,0,4)\) with magnitude 5. The angle between the planes equals the angle between their normals: \(\cos\theta=\dfrac{|(1,2,2)\cdot(3,0,4)|}{3\times5}=\dfrac{11}{15}\), so \(\theta=\) 42.8\(^\circ\) So the planes meet at about \(42.8^\circ\).
Answer to Question 6
Method: the distance from the point \((x_1,y_1,z_1)\) to the plane \(ax+by+cz=d\) is \(\dfrac{|ax_1+by_1+cz_1-d|}{\sqrt{a^2+b^2+c^2}}\). Alternatively, follow the normal line from the point until it meets the plane.
- Substitute the coordinates of \(P\) into the formula. \(\dfrac{|2(2)-2(3)+(-1)-5|}{\sqrt{4+4+1}}=\dfrac{|{-8}|}3=\) \(\dfrac83\) So \(P\) is \(\tfrac83\approx2.67\) units from the plane.
- A line perpendicular to the plane has the normal vector \((2,-2,1)\) as its direction. The normal is the direction: \(\mathbf r=\begin{pmatrix}2\\3\\-1\end{pmatrix}+t\begin{pmatrix}2\\-2\\1\end{pmatrix}\)
- Substitute the general point of the line into the equation of the plane. Substituting: \(2(2+2t)-2(3-2t)+(-1+t)=5\) gives \(4+4t-6+4t-1+t=5\), \(9t=8\), \(t=\tfrac89\). The foot is \(\left(\tfrac{34}9,\tfrac{11}9,-\tfrac19\right)\). Check: \(\tfrac{68}9-\tfrac{22}9-\tfrac19=\tfrac{45}9=5\) β. Check: the distance from \(P\) to the foot is \(\tfrac89\times|(2,-2,1)|=\tfrac89\times3=\tfrac83\), as in part a).
Answer to Question 7
- Speed \(=|\mathbf d|=\sqrt{4+16+1}=\) \(\sqrt{21}\approx4.58\) m s\(^{-1}\).
- The closest point has \(\mathbf r\cdot\mathbf d=0\): \((10+2t)2+(-20+4t)4+(30-t)(-1)=0\), \(20+4t-80+16t-30+t=0\), \(21t=90\), \(t=\) \(\tfrac{30}7\approx4.29\) s.
- \(\mathbf a\times\mathbf d=(-100,70,80)\), magnitude \(\sqrt{21300}=145.9\). Distance \(=\dfrac{145.9}{\sqrt{21}}=\) 31.8 m.
- \(31.8>30\), so the drone does stay at least 30 m away.
Answer to Question 8
- \(\overrightarrow{PQ}=(6,0,0)\), \(\overrightarrow{PR}=(0,4,2)\), product \(=(0\cdot2-0\cdot4,\ 0\cdot0-6\cdot2,\ 6\cdot4-0)=\) \((0,-12,24)\)
- The normal is \((0,-1,2)\). \(\mathbf r\cdot\mathbf n=(0,0,4)\cdot(0,-1,2)=8\), so \(-y+2z=8\). Check \(Q\): \(8\) β, \(R\): \(-4+12=8\) β.
- Area \(=\tfrac12\sqrt{144+576}=\tfrac12\sqrt{720}=\) 13.4 m\(^2\).
- The horizontal has normal \(\mathbf k\). \(\cos\theta=\dfrac{|\mathbf n\cdot\mathbf k|}{|\mathbf n|}=\dfrac2{\sqrt5}\), so \(\theta=\) 26.6\(^\circ\).
Answer to Question 9
- \(\mathbf r=(0,0,9)+\lambda(1,2,-3)\)
- Substitute: \(2\lambda+2\lambda+2(9-3\lambda)=12\), so \(4\lambda+18-6\lambda=12\), \(\lambda=3\). The point is \((3,6,0)\).
- \(\sin\varphi=\dfrac{|(1,2,-3)\cdot(2,1,2)|}{\sqrt{14}\times3}=\dfrac2{3\sqrt{14}}\), so \(\varphi=\) 10.3\(^\circ\) (a shallow angle).
- \((1,2,-2)\cdot(2,1,2)=2+2-4=0\), so the beam is parallel to the mirror and never meets it (the point \(A\) is not on the mirror since \(18\ne12\)).
Answer to Question 10
- Equating: \(1+\lambda=2+2\mu\), \(2-\lambda=\mu\), \(3+2\lambda=-1+\mu\). From the second, \(\mu=2-\lambda\); the first gives \(1+\lambda=6-2\lambda\), \(\lambda=\tfrac53\), \(\mu=\tfrac13\). The third: \(3+\tfrac{10}3=\tfrac{19}3\) but \(-1+\tfrac13=-\tfrac23\). Not equal, so the lines do not meet; they are skew.
- \(\mathbf d_1\times\mathbf d_2=(-3,3,3)\), or \((-1,1,1)\).
- \(\overrightarrow{AB}=(1,-2,-4)\) with \(A\) on \(l_1\) and \(B\) on \(l_2\). \(|\overrightarrow{AB}\cdot\mathbf n|/|\mathbf n|=\dfrac{|-3-6-12|}{\sqrt{27}}=\dfrac{21}{5.196}=\) 4.04 km.
- \(4.04\ge3\), so yes, the requirement is met.
Answer to Question 11
Method: the scalar product is \(\mathbf a\cdot\mathbf b=a_1b_1+a_2b_2+a_3b_3=|\mathbf a||\mathbf b|\cos\theta\). Two non-zero vectors are perpendicular exactly when their scalar product is 0.
- Work done is the scalar product of force and displacement. \(12-2+10=\) 20 J So the crane does 20 J of work.
- Use Pythagoras in three dimensions. \(|\mathbf F|=\sqrt{16+4+25}=\sqrt{45}\approx6.71\) N; \(|\mathbf s|=\sqrt{9+1+4}=\sqrt{14}\approx3.74\) m.
- Use \(\cos\theta=\dfrac{\mathbf F\cdot\mathbf s}{|\mathbf F||\mathbf s|}\). \(\cos\theta=\dfrac{20}{\sqrt{45}\sqrt{14}}=\dfrac{20}{25.1}=0.7968\), so \(\theta=\) 37\(^\circ\) So the force acts at about \(37^\circ\) to the motion.
- The component of \(\mathbf F\) along \(\mathbf s\) is \(\mathbf F\cdot\hat{\mathbf s}=|\mathbf F|\cos\theta\). \(\dfrac{\mathbf F\cdot\mathbf s}{|\mathbf s|}=\dfrac{20}{\sqrt{14}}=\) 5.35 N Check: \(5.35\times\sqrt{14}=20\), the work done.
Answer to Question 12
- \(\mathbf r\times\mathbf F=\left(0\cdot(-10)-0.1\cdot30,\ 0.1\cdot0-0.4\cdot(-10),\ 0.4\cdot30-0\right)=\) \((-3,4,12)\) N m
- \(\sqrt{9+16+144}=\sqrt{169}=\) 13 N m
- The \(z\)-component is 12 N m, which turns the bolt.
- The moment has magnitude \(|\mathbf r||\mathbf F|\sin\theta\), so doubling \(|\mathbf r|\) doubles the turning effect for the same force.
Answer to Question 13
Method: the vector product \(\mathbf a\times\mathbf b\) is perpendicular to both vectors and has magnitude \(|\mathbf a||\mathbf b|\sin\theta\), the area of the parallelogram with sides \(\mathbf a\) and \(\mathbf b\). Compute it as a \(3\times3\) determinant.
- \(\begin{vmatrix}\mathbf i&\mathbf j&\mathbf k\\-1&3&2\\0&-2&4\end{vmatrix}=\mathbf i(12+4)-\mathbf j(-4-0)+\mathbf k(2-0)=\) \((16,4,2)\)
- This scalar triple product gives six times the volume of the tetrahedron. \(\overrightarrow{OA}\cdot(16,4,2)=32+4+0=36\). \(V=\dfrac{36}6=\) 6 m\(^3\). So the tent holds 6 mΒ³ of air.
- The area of the triangle is half the magnitude of the vector product. \(\tfrac12\sqrt{256+16+4}=\tfrac12\sqrt{276}=\) 8.31 m\(^2\).
- Use the volume formula for a pyramid with base \(OBC\). \(V=\tfrac13\times\text{base}\times h\), so \(h=\dfrac{3V}{\text{area}}=\dfrac{18}{8.31}=\) 2.17 m. (Directly: \(\dfrac{36}{\sqrt{276}}=2.17\).) So \(A\) is about 2.17 m from the plane \(OBC\).
Answer to Question 14
- For A: \(1+2\lambda=3\), \(2-\lambda=1\), \(3+\lambda=4\) all give \(\lambda=1\). For B: \(4-\mu=3\), \(-1+2\mu=1\), \(2+2\mu=4\) all give \(\mu=1\). So the paths cross at \((3,1,4)\).
- Both submarines reach that point when \(t=1\), because the parameters are times. So yes, they collide at \(t=1\) hour.
- \(\cos\theta=\dfrac{|(2,-1,1)\cdot(-1,2,2)|}{\sqrt6\times3}=\dfrac{|-2-2+2|}{3\sqrt6}=\dfrac2{3\sqrt6}\), so \(\theta=\) 74.2\(^\circ\)
- A: \(\sqrt{4+1+1}=\sqrt6\approx\) 2.45 km h\(^{-1}\); B: \(\sqrt{1+4+4}=\) 3 km h\(^{-1}\).
Answer to Question 15
- \((1+\lambda)+2\lambda-(2+\lambda)=4\) gives \(2\lambda-1=4\), \(\lambda=\tfrac52\). The point is \(\left(\tfrac72,\tfrac52,\tfrac92\right)\).
- \(\sin\varphi=\dfrac{|1+2-1|}{\sqrt3\sqrt6}=\dfrac2{\sqrt{18}}=0.4714\), so \(\varphi=\) 28.1\(^\circ\)
- At \(P\): \(1+0-2=-1\ne4\). Distance \(=\dfrac{|-1-4|}{\sqrt6}=\dfrac5{\sqrt6}\approx\) 2.04.
- The normal \((1,2,-1)\) points towards the plane (the value \(-5\) is negative, so \(P\) is on the side where \(x+2y-z<4\)). The image is \(P+2\cdot\dfrac56(1,2,-1)=\) \(\left(\tfrac83,\tfrac{10}3,\tfrac13\right)\). Check: the midpoint of \(P\) and its image is \(\left(\tfrac{11}6,\tfrac53,\tfrac76\right)\), which satisfies \(x+2y-z=\tfrac{11}6+\tfrac{20}6-\tfrac76=4\). β
Answer to Question 16
- \(\mathbf w=(2,-1,3)-(1,1,0)=\) \((1,-2,3)\)
- Normal \(=\mathbf d\times\mathbf w=(1,2,1)\times(1,-2,3)=(8,-2,-4)\), or \((4,-1,-2)\). With the point \((1,1,0)\): \(4-1=3\). So \(4x-y-2z=3\). Check \((2,-1,3)\): \(8+1-6=3\) β.
- \(\dfrac{|\mathbf w\times\mathbf d|}{|\mathbf d|}=\dfrac{\sqrt{64+4+16}}{\sqrt6}=\dfrac{\sqrt{84}}{\sqrt6}=\) \(\sqrt{14}\approx3.74\)
- Sliding a point along a line changes \(\mathbf w\) by a multiple of \(\mathbf d\), and \(\mathbf d\times\mathbf d=\mathbf 0\), so the cross product, and hence the distance, is unchanged.
Answer to Question 17
- \(\overrightarrow{AB}=(1+2\mu-\lambda,\ \lambda+\mu-2,\ \mu-2\lambda-4)\)
- \(\mathbf d_1\): \((1+2\mu-\lambda)-(\lambda+\mu-2)+2(\mu-2\lambda-4)=0\) gives \(-6\lambda+3\mu-5=0\). \(\mathbf d_2\): \(2(1+2\mu-\lambda)+(\lambda+\mu-2)+(\mu-2\lambda-4)=0\) gives \(-3\lambda+6\mu-4=0\). Solving: from the first \(\mu=\dfrac{6\lambda+5}3\); substituting, \(-3\lambda+12\lambda+10-4=0\), \(\lambda=-\tfrac23\) and \(\mu=\tfrac13\).
- \(A=\left(\tfrac13,\tfrac83,\tfrac53\right)\), \(B=\left(\tfrac83,\tfrac13,-\tfrac23\right)\). \(\overrightarrow{AB}=\left(\tfrac73,-\tfrac73,-\tfrac73\right)\) and \(|AB|=\tfrac73\sqrt3=\) 4.04.
- \(\dfrac{7\sqrt3}3=4.04\) matches \(\dfrac{21}{\sqrt{27}}=\dfrac{21}{3\sqrt3}=\dfrac{7}{\sqrt3}\). β Also \(\overrightarrow{AB}\parallel(-1,1,1)\), the common perpendicular.
Answer to Question 18
Method: a plane with normal \(\mathbf n\) through the point \(A\) has equation \(\mathbf r\cdot\mathbf n=\mathbf a\cdot\mathbf n\), that is \(n_1x+n_2y+n_3z=d\). A normal to a plane containing two directions is their vector product.
- Intercepts 2, 3, 6: \(\dfrac x2+\dfrac y3+\dfrac z6=1\), or \(3x+2y+z=6\). Check via \(\overrightarrow{AB}\times\overrightarrow{AC}=(18,12,6)\parallel(3,2,1)\).
- \(V=\tfrac16\times2\times3\times6=\) 6.
- \(\tfrac12|\overrightarrow{AB}\times\overrightarrow{AC}|=\tfrac12\sqrt{324+144+36}=\tfrac12\sqrt{504}=\) 11.2
- \(V=\tfrac13\times11.22\times h=6\) gives \(h=\dfrac{18}{11.22}=1.60\). Formula: \(\dfrac{|0-6|}{\sqrt{9+4+1}}=\dfrac6{\sqrt{14}}=1.60\). β
Answer to Question 19
Method: a plane with normal \(\mathbf n\) through the point \(A\) has equation \(\mathbf r\cdot\mathbf n=\mathbf a\cdot\mathbf n\), that is \(n_1x+n_2y+n_3z=d\). A normal to a plane containing two directions is their vector product.
- A normal is perpendicular to both direction vectors of the plane, so take their vector product. \(\begin{vmatrix}\mathbf i&\mathbf j&\mathbf k\\1&1&0\\0&1&1\end{vmatrix}=\mathbf i(1)-\mathbf j(1)+\mathbf k(1)=\) \((1,-1,1)\) Check: \((1,-1,1)\cdot(1,1,0)=0\) and \((1,-1,1)\cdot(0,1,1)=0\).
- Use the point \((1,0,2)\) to find \(d\). \(\mathbf r\cdot\mathbf n=(1,0,2)\cdot(1,-1,1)=3\): \(x-y+z=3\)
- Substitute into the Cartesian equation, then compare components with the vector equation. \(3-1+1=3\) β. Equate: \(1+\lambda=3\) gives \(\lambda=2\); \(\lambda+\mu=1\) gives \(\mu=-1\); \(2+\mu=1\) β. So \(\lambda=2\), \(\mu=-1\). All three equations are consistent, so the point lies in the plane.
- Use: the distance from the point \((x_1,y_1,z_1)\) to the plane \(ax+by+cz=d\) is \(\dfrac{|ax_1+by_1+cz_1-d|}{\sqrt{a^2+b^2+c^2}}\). \(\dfrac{|0-3|}{\sqrt3}=\dfrac3{\sqrt3}=\) \(\sqrt3\approx1.73\)
Answer to Question 20
- Dividing by \(|\mathbf a|^2|\mathbf b|^2\): \(\dfrac{|\mathbf a\times\mathbf b|^2}{|\mathbf a|^2|\mathbf b|^2}=1-\cos^2\theta=\sin^2\theta\). Taking positive square roots (since \(0\le\theta\le\pi\)) gives \(|\mathbf a\times\mathbf b|=|\mathbf a||\mathbf b|\sin\theta\).
- \(|\mathbf a\times\mathbf b|^2=230\). \(|\mathbf a|^2|\mathbf b|^2-(\mathbf a\cdot\mathbf b)^2=14\times21-64=294-64=230\). β
- The left side is \((a_2b_3-a_3b_2)^2+(a_3b_1-a_1b_3)^2+(a_1b_2-a_2b_1)^2\). Expanding gives the sum of terms \(a_i^2b_j^2\) with \(i\ne j\), minus \(2a_ia_jb_ib_j\) over the three pairs. The right side is \((a_1^2+a_2^2+a_3^2)(b_1^2+b_2^2+b_3^2)-(a_1b_1+a_2b_2+a_3b_3)^2\), and the terms \(a_i^2b_i^2\) cancel, leaving the same expression. So the two sides are equal.
- A parallelogram with sides \(\mathbf a\) and \(\mathbf b\) has base \(|\mathbf a|\) and height \(|\mathbf b|\sin\theta\), so its area is \(|\mathbf a||\mathbf b|\sin\theta=|\mathbf a\times\mathbf b|\).
How to use these Further Maths further vectors 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 further vectors lesson again. Finally, check that the method is secure with the quiz or the test.
Also, the Further Maths further vectors 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 further vectors worksheet answers show every step, so nothing is left unexplained.


















