Chapter 11: Vectors
向量 — Magnitude, Direction, Operations, and Motion
| Term 术语 | Chinese 中文 | Meaning |
|---|---|---|
| Scalar | 标量 | Magnitude only (e.g. speed, temperature) |
| Vector | 向量 | Magnitude AND direction (e.g. velocity, force) |
| Component form | 分量形式 | $\vec{v}=\langle v_1, v_2\rangle$ |
| Magnitude | 模长 | $\|\vec{v}\|=\sqrt{v_1^2+v_2^2}$ |
| Unit vector | 单位向量 | Vector with magnitude $1$ |
| Dot product | 点积/标量积 | $\vec{u}\cdot\vec{v}=u_1v_1+u_2v_2$ (scalar result) |
| Resultant force | 合力 | Vector sum of two or more forces |
| Position vector | 位置向量 | $\vec{r}(t)=\langle x(t),y(t)\rangle$ |
| Velocity vector | 速度向量 | Direction and speed of motion |
| Speed | 速率 | Magnitude of velocity vector |
| Normalizing | 单位化 | Finding unit vector: $\hat{u}=\vec{v}/\|\vec{v}\|$ |
11.1 Scalars vs Vectors 标量与向量
Examples: $20\text{ m}$, $50\text{ mph}$, $98.6°F$, mass, time, temperature
Examples: force $60\text{ lbs NE}$, velocity $50\text{ mph East}$, displacement $\langle -4,3\rangle$
- Zero vector(零向量): $\vec{0}=\langle 0,0\rangle$ — no length, no direction
- Equal vectors(相等向量): same magnitude AND direction (can be at different locations)
- Negative vector(相反向量): $-\vec{v}=\langle -v_1,-v_2\rangle$ — same magnitude, opposite direction
11.2 Component Form and Magnitude 分量形式与模长
Point $P$ has coordinates $(3,7)$ and point $Q$ has coordinates $(8,2)$. Find the component form and magnitude of $\overrightarrow{PQ}$.
$\overrightarrow{PQ} = \langle 8-3,\; 2-7\rangle = \langle 5,\,-5\rangle$
$\|\overrightarrow{PQ}\| = \sqrt{5^2+(-5)^2} = \sqrt{25+25} = \sqrt{50} = 5\sqrt{2}$
Direction Angle 方向角
- $\tan^{-1}\frac{b}{a}$ only gives angles between $-90°$ and $90°$. If $a<0$ (Quadrant II or III), add $180°$; if $a>0$ and $b<0$ (Quadrant IV), add $360°$.
- If $a=0$: $\theta=90°$ when $b>0$, and $\theta=270°$ when $b<0$.
Find the magnitude and the direction angle ($0°\le\theta<360°$) of (a) $\langle-3,4\rangle$, (b) $\langle2,-5\rangle$, (c) $\langle-6,-6\rangle$.
11.3 Vector Operations 向量运算
Geometric: head-to-tail method(首尾相接法)
Same as $\vec{u}+(-\vec{v})$
$c>0$: same dir; $c<0$: opposite dir
Result is a scalar(标量)
- 0 · Compare
Place $\vec{u}$ and $\vec{v}$ at one tail. - 1 · Translate
Move $\vec{v}$ to the head of $\vec{u}$. - 2 · Resultant
Connect the first tail to the final head.
Let $\vec{u}=\langle 3,5\rangle$, $\vec{v}=\langle 4,-2\rangle$, and $\vec{w}=\langle -4,5\rangle$. Find $\vec{u}+\vec{v}$. Then find $2\vec{w}$ and $-3\vec{v}$.
$\vec{u}+\vec{v}=\langle 3+4,\;5+(-2)\rangle=\langle 7,3\rangle$
$2\vec{w}=\langle 2(-4),2(5)\rangle=\langle -8,10\rangle$
$-3\vec{v}=\langle -3(4),-3(-2)\rangle=\langle -12,6\rangle$
Let $\vec{u}=\langle 5,6\rangle$, $\vec{v}=\langle -3,2\rangle$. Find $\vec{u}-\vec{v}$.
Let $\vec{a}=\langle 2,-1\rangle$, $\vec{b}=\langle -3,4\rangle$. Compute: (a) $3\vec{a}-2\vec{b}$, (b) $\|\vec{a}+\vec{b}\|$.
(b) $\vec{a}+\vec{b}=\langle-1,3\rangle$; $\|\vec{a}+\vec{b}\|=\sqrt{1+9}=\sqrt{10}$
Parallel Vectors 平行向量
Two nonzero vectors $\vec u=\langle u_1,u_2\rangle$ and $\vec v=\langle v_1,v_2\rangle$ are parallel exactly when $\vec u=c\,\vec v$ for some number $c$; equivalently, $u_1v_2-u_2v_1=0$.
(a) Are $\langle6,-9\rangle$ and $\langle-4,6\rangle$ parallel? If so, do they point in the same or opposite directions?
(b) Find $k$ so that $\langle k,6\rangle$ is parallel to $\langle2,-3\rangle$. (c) Are $\langle3,5\rangle$ and $\langle5,3\rangle$ parallel?
(b) $\langle k,6\rangle=c\langle2,-3\rangle$: $6=-3c\Rightarrow c=-2$, so $k=2c=-4$.
(c) $3(3)-5(5)=-16\neq0$, so they are not parallel.
11.4 Resultant Force 合力
Law of Sines 正弦定理: $\dfrac{a}{\sin A}=\dfrac{b}{\sin B}=\dfrac{c}{\sin C}$
In vector addition diagrams, use the supplementary angle(补角)$180°-\theta$ between the vectors when forming a triangle.
Two forces of $25$ lb and $60$ lb act on a body. The angle between them is $30°$. Find the magnitude of the resultant force and the angle it makes with the smaller force.
In the parallelogram of forces, the diagonal is the resultant. The two sides are $25$ and $60$. The interior angle of the triangle is $180°-30°=150°$.
$R^2 = 25^2+60^2-2(25)(60)\cos150°$
$= 625+3600-3000\cos150°$
$= 4225-3000\!\left(-\dfrac{\sqrt{3}}{2}\right) = 4225+2598.1 = 6823.1$
$R = \sqrt{6823.1}\approx 82.6\text{ lb}$
$\dfrac{\sin\alpha}{60}=\dfrac{\sin150°}{82.6}\Rightarrow \sin\alpha=\dfrac{60\times0.5}{82.6}\approx0.363\Rightarrow\alpha\approx21°$
A plane flies at $534$ mph. Wind blows at $47$ mph at $38°$ to the plane's direction. Find the resultant speed and the angle between the resultant velocity and the wind vector.
$R^2 = 534^2+47^2-2(534)(47)\cos142°$
$= 285156+2209-50196(-0.788)$
$\approx 287365+39554 = 326919$
$R\approx571.8\text{ mph}$
$\dfrac{\sin\beta}{534}=\dfrac{\sin142°}{571.8}\Rightarrow\sin\beta=\dfrac{534\times0.6157}{571.8}\approx0.5752\Rightarrow\beta\approx35.1°$
Resultant by Components 分量法求合力
- Write each vector in components from its magnitude and direction angle: $\langle\|\vec F\|\cos\theta,\;\|\vec F\|\sin\theta\rangle$.
- Add the components.
- Find the magnitude and the direction angle of the sum (check the quadrant).
(a) Two forces act on an object: $\vec F_1$ has magnitude $40$ N and direction angle $30°$; $\vec F_2$ has magnitude $25$ N and direction angle $135°$. Find the magnitude and direction angle of the resultant.
(b) Check the answer to T-6 with the component method.
$\vec F_1=40\langle\cos30°,\sin30°\rangle\approx\langle34.641,\;20\rangle$
$\vec F_2=25\langle\cos135°,\sin135°\rangle\approx\langle-17.678,\;17.678\rangle$
$\vec R\approx\langle16.963,\;37.678\rangle$, $\|\vec R\|=\sqrt{16.963^2+37.678^2}\approx41.320$ N
Quadrant I: $\theta=\tan^{-1}\dfrac{37.678}{16.963}\approx65.8°$.
Check with the Law of Cosines: the angle between the forces is $135°-30°=105°$, so the triangle angle is $75°$: $\;R^2=40^2+25^2-2(40)(25)\cos75°\approx1707.36$, $R\approx41.32$ ✓
Sum $\approx\langle571.037,\;28.936\rangle$: $\|\vec R\|\approx571.8$ mph ✓. Its direction angle is $\tan^{-1}\frac{28.936}{571.037}\approx2.9°$, so the angle between $\vec R$ and the wind is $38°-2.9°\approx35.1°$ ✓.
Vectors $\vec u$ and $\vec v$ have $\|\vec u\|=5$, $\|\vec v\|=8$, and $\|\vec u+\vec v\|=10$. Find (a) the angle $\theta$ between $\vec u$ and $\vec v$; (b) the angle $\alpha$ between $\vec u$ and $\vec u+\vec v$.
$\varphi\approx97.9°$, so $\theta=180°-\varphi\approx82.1°$.
($\alpha$ is acute: only the angle opposite the longest side can be obtuse.)
(a) A boat heads due north at $12$ mph while the current flows due east at $5$ mph. Find the boat's resultant speed and the direction angle of its motion.
(b) Two forces of $30$ N and $50$ N have a resultant of $70$ N. Find the angle between the two forces.
(b) Triangle with sides $30$, $50$, $70$: $\cos\varphi=\dfrac{30^2+50^2-70^2}{2(30)(50)}=\dfrac{-1500}{3000}=-0.5\Rightarrow\varphi=120°$. The angle between the forces is $180°-120°=60°$.
11.5 Dot Product 点积
- Commutative(交换律): $\vec{u}\cdot\vec{v}=\vec{v}\cdot\vec{u}$
- Distributive(分配律): $\vec{u}\cdot(\vec{v}+\vec{w})=\vec{u}\cdot\vec{v}+\vec{u}\cdot\vec{w}$
- Magnitude(模长): $\vec{v}\cdot\vec{v}=\|\vec{v}\|^2$
Geometric Meaning: Perpendicularity 几何意义:垂直
| Dot Product 点积值 | Angle Type 角的类型 | 中文 |
|---|---|---|
| $> 0$ | $0°\le\theta<90°$: acute, or the same direction ($\theta=0°$) | 锐角或同向 |
| $< 0$ | $90°<\theta\le180°$: obtuse, or opposite directions ($\theta=180°$) | 钝角或反向 |
| $= 0$ | $\theta=90°$: perpendicular vectors | 垂直向量 |
Let $\vec{u}=\langle 2,3\rangle$, $\vec{v}=\langle 5,-1\rangle$, $\vec{w}=\langle 4,-2\rangle$. Find: (a) $\vec{u}\cdot\vec{v}$, (b) $\vec{u}\cdot(\vec{v}+\vec{w})$.
$\vec{u}\cdot\vec{v}=2(5)+3(-1)=10-3=7$
$\vec{v}+\vec{w}=\langle5+4,-1+(-2)\rangle=\langle9,-3\rangle$
$\vec{u}\cdot\langle9,-3\rangle=2(9)+3(-3)=18-9=9$
Find $k$ such that $\vec{u}=\langle k,-3\rangle$ and $\vec{v}=\langle 7,-4\rangle$ are perpendicular.
$\vec{u}\cdot\vec{v}=0 \Rightarrow k(7)+(-3)(-4)=0 \Rightarrow 7k+12=0 \Rightarrow k=-\dfrac{12}{7}$
11.6 Angle Between Two Vectors 两向量夹角
Find the angle $\theta$ between $\vec{u}=\langle 3,-5\rangle$ and $\vec{v}=\langle -4,-2\rangle$.
$\vec{u}\cdot\vec{v}=3(-4)+(-5)(-2)=-12+10=-2$
$\|\vec{u}\|=\sqrt{9+25}=\sqrt{34}$; $\|\vec{v}\|=\sqrt{16+4}=\sqrt{20}=2\sqrt{5}$
$\cos\theta=\dfrac{-2}{\sqrt{34}\cdot2\sqrt{5}}=\dfrac{-2}{2\sqrt{170}}=\dfrac{-1}{\sqrt{170}}$
$\theta=\cos^{-1}\!\left(\dfrac{-1}{\sqrt{170}}\right)\approx\cos^{-1}(-0.0767)\approx94.4°$
(a) Find the angle between $\vec{a}=\langle 1,1\rangle$ and $\vec{b}=\langle 1,0\rangle$.
(b) Are $\vec{p}=\langle 6,4\rangle$ and $\vec{q}=\langle -2,3\rangle$ perpendicular?
(b) $\vec{p}\cdot\vec{q}=6(-2)+4(3)=-12+12=0$ → Yes, perpendicular!
11.7 Unit Vectors 单位向量
Vector from magnitude and direction 由大小和方向角求向量: $$\vec{v} = \|\vec{v}\|\langle\cos\theta,\sin\theta\rangle = \|\vec{v}\|\cos\theta\;\mathbf{i}+\|\vec{v}\|\sin\theta\;\mathbf{j}$$
(a) Find a unit vector in the same direction as $\vec{v}=2\mathbf{i}-7\mathbf{j}$.
(b) Find $k$ such that $\left\langle\dfrac{2}{3},k\right\rangle$ is a unit vector.
$\|\vec{v}\|=\sqrt{4+49}=\sqrt{53}$
$\hat{u}=\dfrac{1}{\sqrt{53}}\langle2,-7\rangle=\left\langle\dfrac{2}{\sqrt{53}},\dfrac{-7}{\sqrt{53}}\right\rangle$
$\left(\dfrac{2}{3}\right)^2+k^2=1\Rightarrow\dfrac{4}{9}+k^2=1\Rightarrow k^2=\dfrac{5}{9}\Rightarrow k=\pm\dfrac{\sqrt{5}}{3}$
A ball is thrown at $20$ mph at $45°$ from the positive $x$-axis. Express the velocity vector in terms of $\mathbf{i}$ and $\mathbf{j}$.
In unit vector form: $\vec{v}=10\sqrt{2}\,\mathbf{i}+10\sqrt{2}\,\mathbf{j}$
(a) Express $\langle -3,5\rangle$ in $\mathbf{i},\mathbf{j}$ form and find its length.
(b) Find the unit vector in the direction of $\langle -6,8\rangle$.
(c) Find the vector of magnitude $10$ in the same direction as $\langle 3,4\rangle$, and the vector of magnitude $3$ in the opposite direction.
(b) $\|\vec{v}\|=\sqrt{36+64}=10$; $\hat{u}=\dfrac{1}{10}\langle-6,8\rangle=\langle-0.6,\,0.8\rangle$
(c) Unit vector $\left\langle\frac35,\frac45\right\rangle$; $\;10\left\langle\frac35,\frac45\right\rangle=\langle6,8\rangle$; $\;-3\left\langle\frac35,\frac45\right\rangle=\langle-1.8,\,-2.4\rangle$
11.8 Vector-Valued Functions 向量值函数
An object's position is given by the parametric function $x(t)=t^2-t$, $y(t)=-t+2$, $-3\le t\le3$. Write the position as a vector-valued function (in $\langle\;\rangle$ form and in $\mathbf{i},\mathbf{j}$ form) and find the object's distance from the origin at $t=2$.
$\vec{r}(t)=\langle t^2-t,\;-t+2\rangle=(t^2-t)\,\mathbf{i}+(-t+2)\,\mathbf{j}$
$x(2)=4-2=2$; $y(2)=-2+2=0$. Position: $(2,0)$.
$\|\vec{r}(2)\|=\sqrt{2^2+0^2}=2$
11.9 Velocity and Speed 速度与速率
- $v_x(t)>0$: moving right; $v_x(t)<0$: moving left
- $v_y(t)>0$: moving up; $v_y(t)<0$: moving down
考纲 4.9.A.2 把速度写成 $v(t)=\langle x(t),y(t)\rangle$,那里的 $x(t)$、$y(t)$ 指水平和竖直方向的速度分量,不是位置。本页记作 $v_x(t)$、$v_y(t)$,以免和位置混淆。
A particle has velocity vector $\vec{v}(t)=\langle 2t,\;2t+1\rangle$. At $t=4$, describe the direction of motion and find its speed.
$\vec{v}(4)=\langle 2(4),\;2(4)+1\rangle=\langle 8,9\rangle$
$v_x=8>0$ → moving right; $v_y=9>0$ → moving up. Particle moves up and to the right.
$\text{speed}=\|\vec{v}(4)\|=\sqrt{8^2+9^2}=\sqrt{64+81}=\sqrt{145}\approx12.0$
An object has position $\vec{r}(t)=\langle\cos t,\sin t\rangle$ and its velocity is given by $\vec{v}(t)=\langle -\sin t,\cos t\rangle$. Find the distance from origin and speed at any time $t$.
$\|\vec{r}(t)\|=\sqrt{\cos^2t+\sin^2t}=\sqrt{1}=1$ (constant — always on the unit circle!)
$\|\vec{v}(t)\|=\sqrt{\sin^2t+\cos^2t}=1$ (constant speed 1)
Motion over Time 按区间分析运动
A particle's velocity is $\vec v(t)=\langle t^2-4,\;3-t\rangle$ for $0\le t\le5$.
(a) When is the particle moving right? left? up? down? (b) When is it moving left and up at the same time? (c) Find the speed at $t=0$, $t=2$, and $t=3$. (d) Is the particle ever at rest? (e) Describe the motion at $t=4$, including the speed and the direction angle of the velocity.
| $t$-interval | $v_x=t^2-4$ | $v_y=3-t$ | Motion |
|---|---|---|---|
| $0\le t<2$ | $-$ | $+$ | left & up ↖ |
| $2<t<3$ | $+$ | $+$ | right & up ↗ |
| $3<t\le5$ | $+$ | $-$ | right & down ↘ |
A particle has position $\vec{r}(t)=\langle t^2-4,\; t\rangle$.
(a) Write the position at $t=3$. (b) Find $\|\vec{r}(3)\|$. (c) If velocity is $\vec{v}(t)=\langle 2t,1\rangle$, find the speed at $t=3$ and describe direction of motion.
(b) $\|\vec{r}(3)\|=\sqrt{25+9}=\sqrt{34}$
(c) $\vec{v}(3)=\langle6,1\rangle$; speed $=\sqrt{36+1}=\sqrt{37}\approx6.1$; moving right ($v_x=6>0$) and up ($v_y=1>0$)
Chapter 11 Summary 本章总结
| Operation / Concept | Formula |
|---|---|
| Component form | $\overrightarrow{PQ}=\langle x_2-x_1,\;y_2-y_1\rangle$ |
| Magnitude | $\|\vec{v}\|=\sqrt{v_1^2+v_2^2}$ |
| Addition | $\vec{u}+\vec{v}=\langle u_1+v_1,\;u_2+v_2\rangle$ |
| Subtraction | $\vec{u}-\vec{v}=\langle u_1-v_1,\;u_2-v_2\rangle$ |
| Scalar multiplication | $c\vec{v}=\langle cv_1,cv_2\rangle$ |
| Dot product | $\vec{u}\cdot\vec{v}=u_1v_1+u_2v_2$ (scalar) |
| Dot product & angle | $\vec{u}\cdot\vec{v}=\|\vec{u}\|\|\vec{v}\|\cos\theta$ |
| Perpendicular test | $\vec{u}\perp\vec{v}\iff\vec{u}\cdot\vec{v}=0$ |
| Angle between vectors | $\theta=\cos^{-1}\!\left(\dfrac{\vec{u}\cdot\vec{v}}{\|\vec{u}\|\|\vec{v}\|}\right)$ |
| Unit vector (normalize) | $\hat{u}=\dfrac{\vec{v}}{\|\vec{v}\|}$ |
| Vector from magnitude & direction | $\vec{v}=\|\vec{v}\|\langle\cos\theta,\sin\theta\rangle$ |
| Position vector | $\vec{r}(t)=\langle x(t),y(t)\rangle$ |
| Distance from origin | $\|\vec{r}(t)\|=\sqrt{x(t)^2+y(t)^2}$ |
| Speed | $\|\vec{v}(t)\|=\sqrt{v_x(t)^2+v_y(t)^2}$ |
| Direction angle | $\tan\theta=\frac{b}{a}$; add $180°$ if $a<0$, add $360°$ in Quadrant IV |
| Parallel test | $\vec u=c\,\vec v$, or $u_1v_2-u_2v_1=0$ |
| Resultant by components | Add $\langle\|\vec F\|\cos\theta,\;\|\vec F\|\sin\theta\rangle$ for each force, then find magnitude and angle |
| Angle from magnitudes | Law of Cosines on the triangle with sides $\|\vec u\|$, $\|\vec v\|$, $\|\vec u+\vec v\|$; then $\theta=180°-\varphi$ |
| Vector of magnitude $k$ | $k\,\dfrac{\vec v}{\|\vec v\|}$ |
| Motion from $\vec v(t)$ | Signs of $v_x$, $v_y$ on intervals; at rest only if both are $0$ at the same $t$ |
- 向量加法用分量对应相加,不能混淆水平和竖直分量。
- 点积结果是标量,不是向量——常见错误!
- 判断垂直:点积 $=0$;判断角度:用 $\cos\theta=\dfrac{\vec{u}\cdot\vec{v}}{\|\vec{u}\|\|\vec{v}\|}$。
- 合力题:画出平行四边形,用补角($180°-\theta$)代入余弦定理。
- 速率 $=$ 速度向量的模长(标量,永远 $\ge0$)。
- 求方向角先看分量所在的象限:计算器的 $\tan^{-1}$ 只给出 $-90°$ 到 $90°$ 之间的角。
- 只有两个速度分量在同一时刻都为 $0$,粒子才静止。