← 201-SN4-RE, Linear Algebra and Vector Geometry

Self-check: 201-SN4-RE, Linear Algebra and Vector Geometry

One question per chapter, 12 in all, taken from the course's corrected exercises. Answer the ones you can do and skip those from a chapter you have not seen yet: each answer is checked right away, and the solution opens after.

With your free account, each answer is kept and your dashboard files each chapter: passed the check, or to work on. These are the same questions as on the set pages: an answer given here counts there.

The chapters of the course

In the order of the course.

Chapter 1 · Vectors in space: the three products

This exercise asks for almost no numerical computation: you work with the vectors themselves. Let u⃗\vec{u} and v⃗\vec{v} be two non-zero vectors in space, and θ\theta the angle between them.

b) Check this identity on the vectors u⃗=(2,−1,3)\vec{u}=(2, -1, 3) and v⃗=(1,4,−2)\vec{v}=(1, 4, -2) of Part A.

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b)
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Answer

b) 230+64=294=14×21230+64=294=14\times 21

b) We have u⃗×v⃗=(−10,7,9)\vec{u}\times\vec{v}=(-10, 7, 9) so ∥u⃗×v⃗∥2=230\|\vec{u}\times\vec{v}\|^{2}=230, and u⃗⋅v⃗=−8\vec{u}\cdot\vec{v}=-8 so (u⃗⋅v⃗)2=64(\vec{u}\cdot\vec{v})^{2}=64. The sum is 230+64=294230+64=294. On the other side, ∥u⃗∥2=14\|\vec{u}\|^{2}=14 and ∥v⃗∥2=21\|\vec{v}\|^{2}=21, so ∥u⃗∥2∥v⃗∥2=14×21=294\|\vec{u}\|^{2}\|\vec{v}\|^{2}=14\times 21=294. Both sides are equal: the identity checks out.

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Chapter 2 · Lines and planes in space

Consider the two planes π1:2x−y+2z=0\pi_{1} : 2x-y+2z=0 and π2:x+2y−2z=0\pi_{2} : x+2y-2z=0. Note first that their normal vectors have the same norm, which simplifies everything that follows.

a) Check that ∥n1⃗∥=∥n2⃗∥\|\vec{n_{1}}\|=\|\vec{n_{2}}\|, then compute the distance from the point Q(3,1,0)Q(3, 1, 0) to each of the two planes. What do you notice?

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a)
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Answer

a) Norms 3; 53\frac53 and 53\frac53

a) n1⃗=(2,−1,2)\vec{n_{1}}=(2, -1, 2) and n2⃗=(1,2,−2)\vec{n_{2}}=(1, 2, -2) have norms ∥n1⃗∥=4+1+4=3\|\vec{n_{1}}\|=\sqrt{4+1+4}=3 and ∥n2⃗∥=1+4+4=3\|\vec{n_{2}}\|=\sqrt{1+4+4}=3: they are equal. For Q(3,1,0)Q(3, 1, 0): dist(Q,π1)=∣2(3)−1+0∣3=53\text{dist}(Q,\pi_{1})=\dfrac{|2(3)-1+0|}{3}=\dfrac{5}{3} and dist(Q,π2)=∣3+2(1)−0∣3=53\text{dist}(Q,\pi_{2})=\dfrac{|3+2(1)-0|}{3}=\dfrac{5}{3}. The point QQ is equidistant from the two planes.

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Chapter 3 · Matrices, systems and determinants

Consider the matrices A=(2−130)A=\begin{pmatrix} 2 & -1 \\ 3 & 0 \end{pmatrix} and B=(14−25)B=\begin{pmatrix} 1 & 4 \\ -2 & 5 \end{pmatrix}.

a) Compute A+BA+B and 3A−2B3A-2B.

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Answer

a) A+B=(3315)A+B=\begin{pmatrix}3&3\\1&5\end{pmatrix}, 3A−2B=(4−1113−10)3A-2B=\begin{pmatrix}4&-11\\13&-10\end{pmatrix}

a) A+B=(2+1−1+43−20+5)=(3315)A+B=\begin{pmatrix} 2+1 & -1+4 \\ 3-2 & 0+5 \end{pmatrix}=\begin{pmatrix} 3 & 3 \\ 1 & 5 \end{pmatrix}. For 3A−2B3A-2B: 3A=(6−390)3A=\begin{pmatrix} 6 & -3 \\ 9 & 0 \end{pmatrix} and 2B=(28−410)2B=\begin{pmatrix} 2 & 8 \\ -4 & 10 \end{pmatrix}, so 3A−2B=(4−1113−10)3A-2B=\begin{pmatrix} 4 & -11 \\ 13 & -10 \end{pmatrix}.

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Chapter 4 · Linear systems, Gauss and Gauss-Jordan

A linear system only ever has three possible outcomes. This exercise brings out all three, and each time asks you to recognize them ON the row echelon form.

b) Solve {x+y+z=6x+2y+3z=142x+3y+4z=20\begin{cases} x+y+z=6 \\ x+2y+3z=14 \\ 2x+3y+4z=20 \end{cases} and give the solution set in parametric form.

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b)
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Answer

b) (t−2,8−2t,t)(t-2, 8-2t, t)

b) Augmented matrix [11161231423420]\left[\begin{array}{ccc|c} 1 & 1 & 1 & 6 \\ 1 & 2 & 3 & 14 \\ 2 & 3 & 4 & 20 \end{array}\right]. Apply R2→R2−R1R_{2}\to R_{2}-R_{1}, which gives (0,1,2 ∣ 8)(0, 1, 2\,|\,8), then R3→R3−2R1R_{3}\to R_{3}-2R_{1}, which gives (0,1,2 ∣ 8)(0, 1, 2\,|\,8).

The two new rows are identical, so R3→R3−R2R_{3}\to R_{3}-R_{2} gives (0,0,0 ∣ 0)(0, 0, 0\,|\,0). The row echelon form is [111601280000]\left[\begin{array}{ccc|c} 1 & 1 & 1 & 6 \\ 0 & 1 & 2 & 8 \\ 0 & 0 & 0 & 0 \end{array}\right].

Here the zero row has a ZERO right-hand side, which expresses no contradiction at all: it is the equation 0=00=0, always true, which simply signals a redundant equation. The system is consistent. It has two pivots (columns of xx and yy) for three unknowns, so 3−2=13-2=1 free parameter. The unknown zz, whose column carries no pivot, becomes the parameter.

Set z=tz=t. The second row gives y+2t=8y+2t=8, so y=8−2ty=8-2t. The first gives x+(8−2t)+t=6x+(8-2t)+t=6, that is x=6−8+2t−t=t−2x=6-8+2t-t=t-2.

The solution set is {(t−2,8−2t,t) : t∈R}\{(t-2, 8-2t, t)\ :\ t\in\mathbb{R}\}, INFINITELY many solutions. The whole set must be given: answering with a single particular solution, even a correct one, does not earn the marks.

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Chapter 5 · Determinants and Cramer's rule

Let AA be a square matrix of order 33 about which we only know that det⁡(A)=6\det(A)=6. None of its entries is known.

In each case, give the requested value and justify it by the property used, without ever trying to rebuild AA.

d) Give det⁡(A2)\det(A^{2}), det⁡(A−1)\det(A^{-1}) and det⁡(AT)\det(A^{T}). What would det⁡(A+A)\det(A+A) be?

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d)
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Answer

d) 36; 16\frac16; 6; det⁡(A+A)=48\det(A+A)=48

d) det⁡(A2)=det⁡(A)det⁡(A)=6×6=36\det(A^{2})=\det(A)\det(A)=6\times 6=36, by the property det⁡(AB)=det⁡(A)det⁡(B)\det(AB)=\det(A)\det(B). Since det⁡(A)=6≠0\det(A)=6\neq 0, the matrix AA is invertible and det⁡(A−1)=1det⁡(A)=16\det(A^{-1})=\dfrac{1}{\det(A)}=\dfrac{1}{6}. Finally det⁡(AT)=det⁡(A)=6\det(A^{T})=\det(A)=6.

For det⁡(A+A)\det(A+A): the trap is to write det⁡(A)+det⁡(A)=12\det(A)+\det(A)=12. That is wrong, because the determinant is NOT additive. You have to see that A+A=2AA+A=2A, so det⁡(A+A)=det⁡(2A)=23×6=48\det(A+A)=\det(2A)=2^{3}\times 6=48. Remember the formula that does not exist: det⁡(A+B)≠det⁡(A)+det⁡(B)\det(A+B)\neq\det(A)+\det(B) in general. The determinant is multiplicative, never additive.

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Chapter 6 · Linear combinations, linear dependence and bases

This exercise is about the test for linear independence in R3\mathbb{R}^{3}. Recall that three vectors of R3\mathbb{R}^{3} are linearly independent if and only if the determinant formed by their components is non-zero.

a) Let u⃗=(1,2,−1)\vec{u}=(1, 2, -1), v⃗=(2,−1,3)\vec{v}=(2, -1, 3) and w⃗=(4,3,1)\vec{w}=(4, 3, 1). Show that w⃗\vec{w} is a linear combination of u⃗\vec{u} and v⃗\vec{v}, and conclude about the set {u⃗,v⃗,w⃗}\{\vec{u}, \vec{v}, \vec{w}\}.

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Answer

a) w⃗=2u⃗+v⃗\vec{w}=2\vec{u}+\vec{v}: dependent

a) We look for aa and bb such that au⃗+bv⃗=w⃗a\vec{u}+b\vec{v}=\vec{w}, that is {a+2b=42a−b=3−a+3b=1\begin{cases} a+2b=4 \\ 2a-b=3 \\ -a+3b=1 \end{cases}. The first two give a=4−2ba=4-2b, then 2(4−2b)−b=32(4-2b)-b=3, that is 8−5b=38-5b=3, so b=1b=1 and a=2a=2. Test of the third equation: −2+3(1)=1-2+3(1)=1, it holds. So w⃗=2u⃗+v⃗\vec{w}=2\vec{u}+\vec{v}. Since one of the three vectors is expressed in terms of the other two, the set is linearly DEPENDENT. The dependence relation can also be written in its standard form: 2u⃗+v⃗−w⃗=0⃗2\vec{u}+\vec{v}-\vec{w}=\vec{0}, a zero combination whose coefficients are not all zero.

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Chapter 7 · Vector spaces and subspaces

A vector space is not a set of arrows: it is a set equipped with two operations that obey the axioms. The whole chapter rests on this change of viewpoint.

b) Give a basis of P2P_{2} and its dimension. Same question for M2×2M_{2\times 2}, the set of 2×22\times 2 matrices.

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Answer

b) dim⁡P2=3\dim P_2=3; dim⁡M2×2=4\dim M_{2\times 2}=4

b) Standard basis of P2P_{2}: {1,  x,  x2}\left\{1,\;x,\;x^{2}\right\}. It SPANS P2P_{2}, since every polynomial ax2+bx+cax^{2}+bx+c can be written c⋅1+b⋅x+a⋅x2c\cdot 1+b\cdot x+a\cdot x^{2}; it is LINEARLY INDEPENDENT, since c+bx+ax2=0c+bx+ax^{2}=0 for every xx forces a=b=c=0a=b=c=0 (the zero polynomial has all its coefficients equal to zero). Hence dim⁡P2=3\dim P_{2}=3. For M2×2M_{2\times 2}, the standard basis consists of the four matrices with a single 1 and 0 everywhere else, so dim⁡M2×2=4\dim M_{2\times 2}=4. General rule to remember: dim⁡Pn=n+1\dim P_{n}=n+1 (watch the +1+1, forgotten very often) and dim⁡Mm×n=mn\dim M_{m\times n}=mn.

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Chapter 8 · Linear transformations of the plane

Let R60R_{60} be the matrix of the counterclockwise rotation through 60∘60^{\circ} about the origin. Recall that cos⁡60∘=12\cos 60^{\circ}=\dfrac{1}{2} and sin⁡60∘=32\sin 60^{\circ}=\dfrac{\sqrt{3}}{2}.

The blue arrow shows the direction of the rotation.

−3−2−1123−1123A60°

b) Find the image of the point A(2,0)A(2, 0), and check that the distance to the origin is preserved.

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Answer

b) (1,3)(1, \sqrt3), distance 2

b) R60(20)=(12(2)−32(0)32(2)+12(0))=(13)R_{60}\begin{pmatrix} 2 \\ 0 \end{pmatrix}=\begin{pmatrix} \dfrac{1}{2}(2)-\dfrac{\sqrt{3}}{2}(0) \\[4pt] \dfrac{\sqrt{3}}{2}(2)+\dfrac{1}{2}(0) \end{pmatrix}=\begin{pmatrix} 1 \\ \sqrt{3} \end{pmatrix}. The image is A′(1,3)A'(1, \sqrt{3}), whose distance to the origin is 1+3=2\sqrt{1+3}=2, exactly that of AA. A rotation preserves lengths, and this check should become a reflex.

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Chapter 9 · Eigenvalues and diagonalization

Diagonalizing means rewriting the matrix in the basis of its eigenvectors. The only technical difficulty is keeping the ORDER of the columns.

c) What happens if you swap the two columns of PP without touching DD? Illustrate the problem.

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Answer

c) P′DP′−1=(3−2−14)≠AP'DP'^{-1}=\begin{pmatrix}3&-2\\-1&4\end{pmatrix}\neq A

c) If you swap the columns of PP to get P′=(2−111)P'=\begin{pmatrix}2&-1\\1&1\end{pmatrix} while keeping D=(2005)D=\begin{pmatrix}2&0\\0&5\end{pmatrix}, the equality fails: you would be claiming that (21)\begin{pmatrix}2\\1\end{pmatrix} goes with the eigenvalue 2, when it goes with 5. The calculation confirms it, P′DP′−1=(3−2−14)≠AP'DP'^{-1}=\begin{pmatrix}3&-2\\-1&4\end{pmatrix}\neq A. The rule is therefore strict: the ii-th column of PP must be an eigenvector associated with the ii-th diagonal entry of DD. On the other hand, swapping the columns of PP AND the entries of DD together is perfectly legal and gives another diagonalization, just as valid: diagonalization is not unique, only the PAIRING counts.

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Chapter 10 · Matrix models

A Markov chain describes a system that changes state in steps, with constant probabilities. All the information fits in one matrix, and it is the matrix product that moves time forward.

Two states. Every year, 20% of A move to B and 30% of B move to A.

state Astate B20%30%

c) What does the entry p12p_{12} of the matrix mean?

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Answer

c) From B to A: 0.30.3

c) p12=0.3p_{12}=0.3 is the entry in row 1 and column 2: it is the probability of moving FROM state 2 TO state 1, in other words the share of B that joins A. The order of the indices is the most frequent source of error in the chapter: in the column convention, pijp_{ij} reads “from jj to ii”.

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Chapter 11 · Complex numbers and De Moivre's theorem

Consider the complex number z=−2+2i3z=-2+2i\sqrt{3}.

−5−4−3−2−1123−112345z = −2 + 2i√3

a) Compute ∣z∣|z|, then find arg⁡(z)\arg(z) in radians.

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Answer

a) ∣z∣=4|z|=4, arg⁡z=2π3\arg z=\frac{2\pi}{3}

a) ∣z∣=(−2)2+(23)2=4+12=16=4|z|=\sqrt{(-2)^{2}+(2\sqrt{3})^{2}}=\sqrt{4+12}=\sqrt{16}=4. For the argument, impose BOTH conditions: cos⁡θ=−24=−12\cos\theta=\dfrac{-2}{4}=-\dfrac{1}{2} and sin⁡θ=234=32\sin\theta=\dfrac{2\sqrt{3}}{4}=\dfrac{\sqrt{3}}{2}. A negative cosine and a positive sine put the angle in the second quadrant, and the reference angle for 12\dfrac{1}{2} and 32\dfrac{\sqrt{3}}{2} is π3\dfrac{\pi}{3}. So θ=π−π3=2π3\theta=\pi-\dfrac{\pi}{3}=\dfrac{2\pi}{3}.

The classic pitfall: using the calculator for arctan⁡(23−2)=arctan⁡(−3)=−π3\arctan\left(\dfrac{2\sqrt{3}}{-2}\right)=\arctan(-\sqrt{3})=-\dfrac{\pi}{3}, and stopping there. That value is in the fourth quadrant, while zz is in the second. The arctangent function only ever returns angles between −π2-\dfrac{\pi}{2} and π2\dfrac{\pi}{2}: it cannot tell opposite quadrants apart. Always locate the point before concluding.

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Chapter 12 · Applications in science

A 200200 N light fixture hangs from point OO on two cables attached to a horizontal ceiling. Cable OAOA makes 30∘30^{\circ} with the horizontal, cable OBOB makes 60∘60^{\circ}. Let T1T_{1} and T2T_{2} be the tensions in the two cables, with the xx-axis horizontal to the right and the yy-axis vertical and upward.

ABOT₁T₂30°60°200 N

b) Write the system in the form AX=BAX=B with X=(T1, T2)X=(T_{1},\ T_{2}) and compute det⁡A\det A exactly.

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Answer

b) det⁡A=−sin⁡90∘=−1\det A=-\sin 90^{\circ}=-1

b) A=(−cos⁡30∘cos⁡60∘sin⁡30∘sin⁡60∘)A=\begin{pmatrix} -\cos 30^{\circ} & \cos 60^{\circ} \\ \sin 30^{\circ} & \sin 60^{\circ} \end{pmatrix} and B=(0200)B=\begin{pmatrix} 0 \\ 200 \end{pmatrix}. Then det⁡A=−cos⁡30∘sin⁡60∘−cos⁡60∘sin⁡30∘=−(sin⁡60∘cos⁡30∘+cos⁡60∘sin⁡30∘)=−sin⁡(60∘+30∘)=−sin⁡90∘=−1\det A=-\cos 30^{\circ}\sin 60^{\circ}-\cos 60^{\circ}\sin 30^{\circ}=-(\sin 60^{\circ}\cos 30^{\circ}+\cos 60^{\circ}\sin 30^{\circ})=-\sin(60^{\circ}+30^{\circ})=-\sin 90^{\circ}=-1. The addition formula avoids every decimal, and the exact result −1-1 comes from the two cables being PERPENDICULAR, 30∘+60∘=90∘30^{\circ}+60^{\circ}=90^{\circ}.

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