Unit 9: Parametric Equations,
Polar Coordinates & Vector-Valued Functions
单元 9:参数方程、
极坐标与向量值函数
Extend calculus to curves in the plane — parametric & polar derivatives, arc length, vector motion, and polar areas. BC Only.
将微积分扩展到平面曲线 —— 参数方程与极坐标的导数、弧长、向量运动以及极坐标面积。仅 BC。
Defining and Differentiating Parametric Equations
参数方程(parametric equations)的定义与求导
parametric curve)由 $x = f(t)$ 与 $y = g(t)$ 定义,其中 $t$ 是参数(parameter)。每一个 $t$ 值对应曲线上的一个点 $(x, y)$。
The slope of the tangent line to a parametric curve is found using the chain rule:
参数曲线切线(tangent line)的斜率(slope)通过链式法则(chain rule)得到:
provided $\frac{dx}{dt} \neq 0$
前提是 $\frac{dx}{dt} \neq 0$
Worked Example
例题
Given: x = t² + 1, y = t³ − 3t Find dy/dx at t = 2. dx/dt = 2t → at t=2: dx/dt = 4 dy/dt = 3t² − 3 → at t=2: dy/dt = 9 dy/dx = 9/4
已知:x = t² + 1,y = t³ − 3t 求 t = 2 处的 dy/dx。 dx/dt = 2t → 当 t=2 时:dx/dt = 4 dy/dt = 3t² − 3 → 当 t=2 时:dy/dt = 9 dy/dx = 9/4
Worked Example — Locating Horizontal and Vertical Tangents例题 —— 求水平切线与垂直切线
Given: x = t³ − 3t, y = t² for −2 ≤ t ≤ 2. Find every value of t where the curve has a horizontal or vertical tangent. dx/dt = 3t² − 3 = 3(t² − 1) dy/dt = 2t Horizontal tangent: dy/dt = 0 and dx/dt ≠ 0 2t = 0 → t = 0. Check dx/dt at t=0: 3(0−1) = −3 ≠ 0. ✓ valid. Vertical tangent: dx/dt = 0 and dy/dt ≠ 0 3(t² − 1) = 0 → t = ±1. Check dy/dt: at t=1, dy/dt=2≠0; at t=−1, dy/dt=−2≠0. ✓ both valid. So: horizontal tangent at t=0; vertical tangents at t=1 and t=−1.
已知:x = t³ − 3t,y = t²,其中 −2 ≤ t ≤ 2。 求曲线上所有具有水平切线或垂直切线的 t 值。 dx/dt = 3t² − 3 = 3(t² − 1) dy/dt = 2t 水平切线:dy/dt = 0 且 dx/dt ≠ 0 2t = 0 → t = 0。检验 t=0 处 dx/dt:3(0−1) = −3 ≠ 0。✓ 有效。 垂直切线:dx/dt = 0 且 dy/dt ≠ 0 3(t² − 1) = 0 → t = ±1。检验 dy/dt:t=1 时 dy/dt=2≠0;t=−1 时 dy/dt=−2≠0。✓ 均有效。 结论:t=0 处水平切线;t=1 与 t=−1 处垂直切线。
The check step is not optional: if dy/dt and dx/dt were both zero at the same $t$, the curve would have a cusp or a discontinuity there instead of a genuine tangent, and the point must be examined separately (e.g. with a limit of the slope).
检验步骤并非可有可无:若某个 $t$ 处 dy/dt 与 dx/dt 同时为零,则曲线在该处可能出现尖点或不连续,而非真正的切线,需要单独分析(例如用斜率的极限)。
Worked Example — From Slope to a Full Tangent Line Equation例题 —— 从斜率到完整的切线方程
Same curve as the very first example: x = t² + 1, y = t³ − 3t. Write an equation for the line tangent to the curve at t = 2. The slope alone was already found above: dy/dx = 9/4 at t = 2. On the AP exam, a slope by itself is not a full answer: the line equation needs a point too, so plug t = 2 into BOTH x(t) and y(t): x(2) = 2² + 1 = 5 y(2) = 2³ − 3(2) = 8 − 6 = 2 Assemble point-slope form from the point (5, 2) and slope 9/4: y − 2 = (9/4)(x − 5)
沿用最初的例子:x = t² + 1,y = t³ − 3t。 求曲线在 t = 2 处的切线方程。 上面已求出斜率:t = 2 处 dy/dx = 9/4。 在 AP 考试中,只给出斜率并不是完整答案,切线方程还需要一个点, 所以把 t = 2 同时代入 x(t) 与 y(t): x(2) = 2² + 1 = 5 y(2) = 2³ − 3(2) = 8 − 6 = 2 用点 (5, 2) 与斜率 9/4 写出点斜式: y − 2 = (9/4)(x − 5)
Free-response graders look for the equation itself, point and slope combined into one statement; stopping at "$\frac{dy}{dx} = \frac{9}{4}$" earns only partial credit even though it is the harder half of the work. Whenever a question says "write an equation for the tangent line," treat finding the slope as step one of two, not the whole task.
自由作答题的评分标准要看到完整的方程,把点和斜率写在同一个表达式里;只停留在"$\frac{dy}{dx} = \frac{9}{4}$"通常只能拿到部分分,尽管这一步其实是更难的部分。只要题目问的是"写出切线方程",就应该把求斜率当作两步中的第一步,而不是全部任务。
Second Derivatives of Parametric Equations
参数方程的二阶导数(second derivative)
To find the concavity of a parametric curve, compute the second derivative $\frac{d^2y}{dx^2}$.
要判断参数曲线的凹凸性,需要计算二阶导数 $\frac{d^2y}{dx^2}$。
Step-by-Step Process
分步流程
Step 1: Find $\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}$
第 1 步:求 $\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}$
Step 2: Differentiate $\frac{dy}{dx}$ with respect to $t \rightarrow$ get $\frac{d}{dt}\left(\frac{dy}{dx}\right)$
第 2 步:对 $\frac{dy}{dx}$ 关于 $t$ 求导 $\rightarrow$ 得到 $\frac{d}{dt}\left(\frac{dy}{dx}\right)$
Step 3: Divide by $\frac{dx}{dt} \rightarrow \frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}$
第 3 步:再除以 $\frac{dx}{dt}$ $\rightarrow$ $\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}$
Worked Example — Second Derivative例题 —— 二阶导数
Given: x = t², y = t³ Step 1: dy/dx = (3t²)/(2t) = 3t/2 Step 2: d/dt [3t/2] = 3/2 Step 3: d²y/dx² = (3/2) / (2t) = 3/(4t) At t = 1: d²y/dx² = 3/4 > 0 → concave up
已知:x = t²,y = t³ 第 1 步: dy/dx = (3t²)/(2t) = 3t/2 第 2 步: d/dt [3t/2] = 3/2 第 3 步: d²y/dx² = (3/2) / (2t) = 3/(4t) 当 t = 1:d²y/dx² = 3/4 > 0 → 凹向上
Finding Arc Lengths of Parametric Curves
参数曲线的弧长(arc length)
speed)。对速率沿时间积分,得到的就是总路程(即弧长)。
Worked Example — Arc Length例题 —— 弧长
Find the length of the curve x = 3t, y = 4t, for 0 ≤ t ≤ 5. dx/dt = 3, dy/dt = 4 L = ∫₀⁵ √(9 + 16) dt = ∫₀⁵ 5 dt = 25 (This is just a line segment of length 25 — makes sense!)
求曲线 x = 3t、y = 4t 在 0 ≤ t ≤ 5 上的长度。 dx/dt = 3,dy/dt = 4 L = ∫₀⁵ √(9 + 16) dt = ∫₀⁵ 5 dt = 25 (这就是一段长度为 25 的线段 —— 合情合理!)
Worked Example — Arc Length of a Curved (Non-Linear) Path例题 —— 曲线(非直线)路径的弧长
Find the length of x = t², y = (2/3)t³ for 0 ≤ t ≤ 2. dx/dt = 2t, dy/dt = 2t² Set up the integrand: √((2t)² + (2t²)²) = √(4t² + 4t⁴) = 2t·√(1 + t²) (t ≥ 0 on this interval, so √(t²) = t) Substitute u = 1 + t², du = 2t dt — this cancels the 2t out front exactly: L = ∫₀² 2t√(1+t²) dt = ∫₁⁵ √u du = [ (2/3)u^(3/2) ]₁⁵ = (2/3)(5√5 − 1) ≈ 7.29
求 x = t²、y = (2/3)t³ 在 0 ≤ t ≤ 2 上的长度。 dx/dt = 2t,dy/dt = 2t² 列出被积函数: √((2t)² + (2t²)²) = √(4t² + 4t⁴) = 2t·√(1 + t²) (此区间 t ≥ 0,故 √(t²) = t) 令 u = 1 + t²,du = 2t dt —— 恰好消去前面的 2t: L = ∫₀² 2t√(1+t²) dt = ∫₁⁵ √u du = [ (2/3)u^(3/2) ]₁⁵ = (2/3)(5√5 − 1) ≈ 7.29
Unlike the straight-line example above, this integrand does not simplify to a constant — most AP arc-length integrals are evaluated numerically on a calculator, but recognizing the $u$-substitution here (when it is available) turns a calculator problem into an exact closed form, which is worth checking for before reaching for technology.
与上面的直线例子不同,此被积函数不能化简为常数——大多数 AP 弧长积分需用计算器数值求值,但若能识别出此处可用的 $u$ 替换,就能把计算器题变为精确的闭式解,值得在诉诸计算器前先检查一下。
Defining and Differentiating Vector-Valued Functions
向量值函数(vector-valued function)的定义与求导
position)。
Differentiation works component-wise:
求导按分量逐一进行:
The derivative $\mathbf{r}'(t)$ gives the velocity vector $\mathbf{v}(t)$. Its direction is tangent to the curve at that point.
导数 $\mathbf{r}'(t)$ 即为速度向量(velocity vector) $\mathbf{v}(t)$。它的方向(direction)与曲线在该点处的切线相切。
planar motion)。记号不同,但微积分的内容完全一样。
Worked Example — Velocity and Speed from a Position Vector例题 —— 由位置向量求速度与速率
Given: r(t) = ⟨t² − 1, 2t + 3⟩. Find the velocity vector and speed at t = 2. Differentiate component-wise: r'(t) = ⟨2t, 2⟩ → at t = 2: r'(2) = ⟨4, 2⟩ Speed is the magnitude of the velocity vector: |r'(2)| = √(4² + 2²) = √20 = 2√5 The vector ⟨4, 2⟩ also gives the direction of motion — tangent to the curve at t = 2.
已知:r(t) = ⟨t² − 1, 2t + 3⟩。求 t = 2 时的速度向量与速率。 按分量求导: r'(t) = ⟨2t, 2⟩ → 当 t = 2 时: r'(2) = ⟨4, 2⟩ 速率是速度向量的模: |r'(2)| = √(4² + 2²) = √20 = 2√5 向量 ⟨4, 2⟩ 同时给出了运动方向 —— 即曲线在 t = 2 处的切线方向。
Integrating Vector-Valued Functions
向量值函数的积分(integral)
Integration also works component-wise:
积分同样按分量逐一进行:
Worked Example — Vector IVP例题 —— 向量初值问题
Given: r'(t) = ⟨2t, eᵗ⟩, r(0) = ⟨3, 1⟩ Integrate component-wise: x(t) = t² + C₁ y(t) = eᵗ + C₂ Apply initial conditions r(0) = ⟨3, 1⟩: x(0) = 0 + C₁ = 3 → C₁ = 3 y(0) = 1 + C₂ = 1 → C₂ = 0 Solution: r(t) = ⟨t² + 3, eᵗ⟩
已知:r'(t) = ⟨2t, eᵗ⟩,r(0) = ⟨3, 1⟩ 按分量积分: x(t) = t² + C₁ y(t) = eᵗ + C₂ 代入初始条件 r(0) = ⟨3, 1⟩: x(0) = 0 + C₁ = 3 → C₁ = 3 y(0) = 1 + C₂ = 1 → C₂ = 0 解: r(t) = ⟨t² + 3, eᵗ⟩
Solving Motion Problems — Parametric & Vector-Valued
求解运动问题 —— 参数方程与向量值函数
| Quantity量 | Formula公式 |
|---|---|
| Position位置 | $\mathbf{r}(t) = \langle x(t), y(t) \rangle$ |
| Velocity速度 | $\mathbf{v}(t) = \langle x'(t), y'(t) \rangle$ |
| Speed速率 | $|\mathbf{v}(t)| = \sqrt{(x'(t))^2 + (y'(t))^2}$ |
| Acceleration加速度 | $\mathbf{a}(t) = \langle x''(t), y''(t) \rangle$ |
| Displacement位移 | $\int_{a}^{b} \mathbf{v}(t) dt = \left\langle \int_{a}^{b} x'(t) dt, \int_{a}^{b} y'(t) dt \right\rangle$ |
| Total Distance总路程 | $\int_{a}^{b} |\mathbf{v}(t)| dt \quad$ (Arc Length)(即弧长) |
magnitude)积分得到路程。
acceleration vector)"方向一致"时,速率在增加 —— 具体来说,就是点积 $\mathbf{v}(t) \cdot \mathbf{a}(t) > 0$。当 $\mathbf{v}(t) \cdot \mathbf{a}(t) < 0$ 时,速率在减小。
particle)以速度 $\mathbf{v}(t) = \langle 3, 4 \rangle$ 运动,其速率是多少?Worked Example — Is Speed Increasing or Decreasing?例题 —— 速率是在增加还是减小
A particle moves with x(t) = t² − 4t and y(t) = t³ − 3t. Is speed increasing or decreasing at t = 1? x'(t) = 2t − 4 → x'(1) = −2 y'(t) = 3t² − 3 → y'(1) = 0 x''(t) = 2 y''(t) = 6t → y''(1) = 6 Test the sign of v(t) · a(t): v(1)·a(1) = (−2)(2) + (0)(6) = −4 + 0 = −4 < 0 Negative dot product ⇒ speed is DECREASING at t = 1.
质点满足 x(t) = t² − 4t,y(t) = t³ − 3t。求 t = 1 时速率 是在增加还是减小。 x'(t) = 2t − 4 → x'(1) = −2 y'(t) = 3t² − 3 → y'(1) = 0 x''(t) = 2 y''(t) = 6t → y''(1) = 6 检验 v(t) · a(t) 的符号: v(1)·a(1) = (−2)(2) + (0)(6) = −4 + 0 = −4 < 0 点积为负 ⇒ t = 1 时速率在减小。
This dot-product test is the 2D analogue of the familiar 1D rule "speed increases when velocity and acceleration have the same sign." Here it is applied component-by-component and summed, exactly like any other dot product — no need to separately compute the speed function and differentiate it.
这一点积判别法是一维中"速度与加速度同号时速率增加"这一熟悉规则的二维类比。此处逐分量相乘再求和,与任何其他点积计算方式完全一致——无需另外求出速率函数再对其求导。
Worked Example — Total Distance vs. Displacement例题 —— 总路程与位移
A particle moves with velocity v(t) = ⟨2, 3t² − 3⟩ for 0 ≤ t ≤ 2. Find (a) displacement in y and (b) total distance traveled in y. (a) Displacement — integrate the velocity component directly: ∫₀² (3t² − 3) dt = [t³ − 3t]₀² = (8 − 6) − 0 = 2 (b) Distance — first check if the y-velocity changes sign on [0,2]: 3t² − 3 = 0 → t = 1 (velocity is negative on [0,1], positive on [1,2]) Split the integral and take absolute value of each piece: ∫₀¹ |3t² − 3| dt + ∫₁² |3t² − 3| dt = 2 + 4 = 6 Distance (6) > |displacement| (2) because the particle reversed direction — this only happens when velocity changes sign.
质点以 v(t) = ⟨2, 3t² − 3⟩ 运动,0 ≤ t ≤ 2。 求 (a) y 方向的位移,(b) y 方向的总路程。 (a) 位移 —— 直接对速度分量积分: ∫₀² (3t² − 3) dt = [t³ − 3t]₀² = (8 − 6) − 0 = 2 (b) 路程 —— 先检查 y 方向速度在 [0,2] 上是否变号: 3t² − 3 = 0 → t = 1([0,1] 上速度为负,[1,2] 上为正) 分段积分,每段取绝对值: ∫₀¹ |3t² − 3| dt + ∫₁² |3t² − 3| dt = 2 + 4 = 6 路程(6)大于 |位移|(2),因为质点中途改变了方向 —— 只有速度变号时才会出现这种情况。
Defining Polar Coordinates & Differentiating in Polar Form
极坐标(polar coordinate)的定义与极坐标求导
pole)出发的有向距离(极径,radius),$\theta$ 是从极轴(polar axis)量起的角度(极角,angle)。极坐标与直角坐标的转换:$x = r\cos(\theta)$,$y = r\sin(\theta)$。
A polar curve $r = f(\theta)$ is a special case of parametric equations where $\theta$ is the parameter:
极坐标曲线(polar curve)$r = f(\theta)$ 是参数方程的特殊情形,其中 $\theta$ 担任参数:
$x(\theta) = f(\theta)\cos(\theta)$
$y(\theta) = f(\theta)\sin(\theta)$
Derivative in Polar
极坐标下的导数
Worked Example — Slope of a Polar Curve例题 —— 极坐标曲线的斜率
Find dy/dx for r = 1 + sin(θ) at θ = π/2. Set up x(θ) and y(θ): x = r cos(θ) = (1 + sin θ) cos θ y = r sin(θ) = (1 + sin θ) sin θ Differentiate each with the product rule: dx/dθ = cos(θ)·cos(θ) + (1+sin θ)·(−sin θ) = cos²θ − sinθ − sin²θ dy/dθ = cos(θ)·sin(θ) + (1+sin θ)·cos(θ) = sinθ cosθ + cosθ + sinθ cosθ Evaluate at θ = π/2 (cos = 0, sin = 1): dx/dθ = 0 − 1 − 1 = −2 dy/dθ = 0 + 0 + 0 = 0 dy/dx = 0 / (−2) = 0 (a horizontal tangent — the top of the cardioid)
求 r = 1 + sin(θ) 在 θ = π/2 处的 dy/dx。 先写出 x(θ) 与 y(θ): x = r cos(θ) = (1 + sin θ) cos θ y = r sin(θ) = (1 + sin θ) sin θ 分别用乘积法则求导: dx/dθ = cos(θ)·cos(θ) + (1+sin θ)·(−sin θ) = cos²θ − sinθ − sin²θ dy/dθ = cos(θ)·sin(θ) + (1+sin θ)·cos(θ) = sinθ cosθ + cosθ + sinθ cosθ 代入 θ = π/2(cos = 0,sin = 1): dx/dθ = 0 − 1 − 1 = −2 dy/dθ = 0 + 0 + 0 = 0 dy/dx = 0 / (−2) = 0 (水平切线 —— 心脏线的顶点)
Worked Example — Tangent Line at the Pole例题 —— 极点处的切线
Find the tangent line to r = sin(2θ) at the pole, for the petal that begins at θ = 0. r = 0 when sin(2θ) = 0, so θ = 0 is a pole angle for this petal. Shortcut check: r'(θ) = 2cos(2θ), so r'(0) = 2 ≠ 0, meaning the shortcut applies. Tangent line at the pole: θ = 0, i.e. slope = tan(0) = 0 Verify with the full quotient, x = sin(2θ)cos(θ), y = sin(2θ)sin(θ): dx/dθ = 2cos(2θ)cos(θ) − sin(2θ)sin(θ) → at θ=0: 2(1)(1) − 0 = 2 dy/dθ = 2cos(2θ)sin(θ) + sin(2θ)cos(θ) → at θ=0: 2(1)(0) + 0(1) = 0 dy/dx = 0/2 = 0 ✓ matches the shortcut exactly
求 r = sin(2θ) 在极点处的切线,取从 θ = 0 开始的花瓣。 当 sin(2θ) = 0 时 r = 0,故此花瓣对应的极点角为 θ = 0。 捷径检验:r'(θ) = 2cos(2θ),故 r'(0) = 2 ≠ 0,捷径可用。 极点处切线:θ = 0,即斜率 = tan(0) = 0 用完整商式验证,x = sin(2θ)cos(θ),y = sin(2θ)sin(θ): dx/dθ = 2cos(2θ)cos(θ) − sin(2θ)sin(θ) → θ=0 时:2(1)(1) − 0 = 2 dy/dθ = 2cos(2θ)sin(θ) + sin(2θ)cos(θ) → θ=0 时:2(1)(0) + 0(1) = 0 dy/dx = 0/2 = 0 ✓ 与捷径结果完全一致
The full quotient always agrees with the shortcut when $r'(\theta_0) \neq 0$, so on the exam it is faster and equally rigorous to jump straight to $\tan(\theta_0)$ once you have confirmed the curve actually reaches the pole at that angle.
只要 $r'(\theta_0) \neq 0$,完整商式的结果必然与捷径一致,所以在考试中,一旦确认曲线在该角度确实经过极点,直接跳到 $\tan(\theta_0)$ 既更快,也同样严谨。
Area of a Polar Region — Single Curve
极坐标区域的面积 —— 单曲线
Worked Example — Area of One Petal of $r = \cos(2\theta)$例题 —— 求 $r = \cos(2\theta)$ 一个花瓣的面积
r = cos(2θ) is a rose with 4 petals. One petal: from θ = −π/4 to θ = π/4 (where r ≥ 0). A = ½ ∫−π/4π/4 [cos(2θ)]² dθ Use identity: cos²(u) = (1 + cos(2u))/2 A = ½ ∫−π/4π/4 (1 + cos(4θ))/2 dθ = ¼ [θ + sin(4θ)/4]−π/4π/4 A = ¼ [(π/4 + 0) − (−π/4 + 0)] = ¼ · π/2 = π/8
r = cos(2θ) 是一个 4 瓣玫瑰线。 一个花瓣:θ 从 −π/4 到 π/4(此时 r ≥ 0)。 A = ½ ∫−π/4π/4 [cos(2θ)]² dθ 用恒等式:cos²(u) = (1 + cos(2u))/2 A = ½ ∫−π/4π/4 (1 + cos(4θ))/2 dθ = ¼ [θ + sin(4θ)/4]−π/4π/4 A = ¼ [(π/4 + 0) − (−π/4 + 0)] = ¼ · π/2 = π/8
Area Between Two Polar Curves
两条极坐标曲线之间的面积
Worked Example — Area Inside One Curve and Outside Another例题 —— 一条曲线内、另一条曲线外的面积
Find the area inside r = 2 and outside r = 2 − 2sin(θ). Step 1 — Find intersections by setting the curves equal: 2 = 2 − 2sin(θ) → sin(θ) = 0 → θ = 0, π Step 2 — On this interval, check which curve is outer. At θ = π/2: r = 2 − 2sin(π/2) = 0, so r = 2 (the circle) is outer. Step 3 — Apply the formula, outer² − inner², over the interval where r=2 is outer (0 to π): A = ½ ∫₀π [2² − (2 − 2sinθ)²] dθ Expand (2 − 2sinθ)² = 4 − 8sinθ + 4sin²θ: A = ½ ∫₀π [4 − (4 − 8sinθ + 4sin²θ)] dθ = ½ ∫₀π [8sinθ − 4sin²θ] dθ This integrates (using sin²θ = (1−cos2θ)/2) to: A = 4π − 2π = 2π (exact intermediate steps omitted — set up is the graded skill)
求 r = 2 内部、r = 2 − 2sin(θ) 外部的面积。 第 1 步 —— 令两曲线相等,求交点: 2 = 2 − 2sin(θ) → sin(θ) = 0 → θ = 0, π 第 2 步 —— 在该区间上检查哪条曲线在外。 当 θ = π/2 时:r = 2 − 2sin(π/2) = 0,所以 r = 2(圆)在外。 第 3 步 —— 在 r=2 为外曲线的区间(0 到 π)上代入"外² − 内²": A = ½ ∫₀π [2² − (2 − 2sinθ)²] dθ 展开 (2 − 2sinθ)² = 4 − 8sinθ + 4sin²θ: A = ½ ∫₀π [4 − (4 − 8sinθ + 4sin²θ)] dθ = ½ ∫₀π [8sinθ − 4sin²θ] dθ 用 sin²θ = (1−cos2θ)/2 积分,得: A = 4π − 2π = 2π (省略了具体积分步骤 —— 正确列式才是本题考查的核心技能)
Worked Example — Finding the Hidden Intersection at the Pole例题 —— 找出隐藏在极点处的交点
Curves: r₁ = 2cos(θ), r₂ = 2sin(θ), two circles of radius 1, one centered on the x-axis, one on the y-axis, both through the origin. Find every intersection point. Step 1, set the expressions equal: 2cos(θ) = 2sin(θ) → tan(θ) = 1 → θ = π/4 (in [0, 2π)) At θ = π/4: r = 2cos(π/4) = √2 Step 2, check the pole separately, don't skip this: r₁ = 2cos(θ) = 0 at θ = π/2 r₂ = 2sin(θ) = 0 at θ = 0 Both curves reach r = 0, just at different θ values, so the pole IS a shared point, even though θ = π/2 and θ = 0 never solve r₁ = r₂. Conclusion: TWO intersection points total, (√2, π/4), found algebraically, and the pole, found by the separate check.
曲线:r₁ = 2cos(θ),r₂ = 2sin(θ),两个半径为 1 的圆, 一个圆心在 x 轴上,一个在 y 轴上,都经过原点。 求所有交点。 第 1 步,令两表达式相等: 2cos(θ) = 2sin(θ) → tan(θ) = 1 → θ = π/4(在 [0, 2π) 内) θ = π/4 时: r = 2cos(π/4) = √2 第 2 步,单独检查极点,这一步不能省略: r₁ = 2cos(θ) = 0 于 θ = π/2 r₂ = 2sin(θ) = 0 于 θ = 0 两条曲线都能达到 r = 0,只是 θ 值不同,所以极点确实是两条曲线的 公共点,即使 θ = π/2 与 θ = 0 从未同时满足 r₁ = r₂。 结论:共有两个交点, (√2, π/4),由代数求出;以及极点,由单独检查求出。
A student who only solves $r_1 = r_2$ finds one of the two intersections and would then set up an area-between-curves integral with the wrong bounds, since the missing pole intersection is often exactly where the "outer" and "inner" curve swap roles.
如果只解 $r_1 = r_2$,就只能找到两个交点中的一个,接下来列出的两曲线间面积积分很可能用错边界,因为遗漏的这个极点交点往往正是"外曲线"与"内曲线"互换角色的位置。
How Unit 9 Appears on the AP Exam
单元 9 在 AP 考试中的考法
Find $\frac{dy}{dx}$ for a parametric curve at a specific t-value.
在指定的 t 值处求 $\frac{dy}{dx}$(参数曲线)。
Set up an arc length or polar area integral (frequently without evaluating).
列出弧长或极坐标面积的积分(常常无需求值)。
Determine speed, velocity, or acceleration from vector components.
由向量分量求速率、速度或加速度。
Identify horizontal/vertical tangents on parametric curves.
判断参数曲线上的水平切线或垂直切线。
Particle in the plane: Given velocity components, find position, speed, total distance, or acceleration. Heavily involves initial value problems.
平面内的质点:给出速度分量,求位置、速率、总路程或加速度。这类题往往涉及初值问题。
Polar area: Set up and evaluate area integrals, often between two curves or for one petal of a rose.
极坐标面积:列出并计算面积积分,常见的是两条曲线之间的面积,或玫瑰线一个花瓣的面积。
Flashcards — Click to Flip
闪卡 —— 点击翻面
$$ \frac{\frac{dy}{dt}}{\frac{dx}{dt}} $$
provided $\frac{dx}{dt} \neq 0$前提 $\frac{dx}{dt} \neq 0$
$$ \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}} $$
NOT quotient of 2nd derivatives.不是两个二阶导数相除。
$$ \int_{a}^{b} \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} dt $$
$$ |\mathbf{v}(t)| = \sqrt{(x'(t))^2 + (y'(t))^2} $$
$$ A = \frac{1}{2} \int_{\alpha}^{\beta} [r(\theta)]^2 d\theta $$
When $\mathbf{v}(t) \cdot \mathbf{a}(t) > 0$
(Velocity and acceleration agree)当 $\mathbf{v}(t) \cdot \mathbf{a}(t) > 0$ 时
(速度与加速度方向一致)
Unit 9 — Practice Quiz
单元 9 —— 练习测验
Readiness Checklist
备考清单
Click each item you've mastered. Aim for 100% before exam day.
点击你已经掌握的每一项。考试前争取做到 100%。
- Find $\frac{dy}{dx}$ for a parametric curve using $\frac{dy/dt}{dx/dt}$用 $\frac{dy/dt}{dx/dt}$ 求参数曲线的 $\frac{dy}{dx}$
- Find $\frac{d^2y}{dx^2}$ correctly (not by dividing second derivatives)正确求出 $\frac{d^2y}{dx^2}$(不是用两个二阶导数相除)
- Identify horizontal and vertical tangent lines on parametric curves识别参数曲线上的水平切线与垂直切线
- Set up and evaluate parametric arc length integrals列出并计算参数曲线的弧长积分
- Differentiate and integrate vector-valued functions component-wise按分量对向量值函数求导与积分
- Solve vector initial value problems (position from velocity + initial condition)解向量初值问题(由速度与初始条件求位置)
- Compute speed, displacement, and total distance from velocity components由速度分量求速率、位移与总路程
- Determine when speed is increasing vs. decreasing ($\mathbf{v} \cdot \mathbf{a}$)用 $\mathbf{v} \cdot \mathbf{a}$ 判断速率递增或递减
- Find position at a later time using $\int$ of velocity components用速度分量的 $\int$ 求之后时刻的位置
- Compute acceleration magnitude and direction from vector components由向量分量求加速度的模与方向
- Convert between polar and rectangular coordinates在极坐标与直角坐标之间互相转换
- Sketch a polar curve and identify its symmetry画出极坐标曲线并判断其对称性
- Find $\frac{dy}{dx}$ for a polar curve using the product rule使用乘积法则求极坐标曲线的 $\frac{dy}{dx}$
- Set up and evaluate polar area integrals (single curve and between two curves)列出并计算极坐标面积积分(单曲线与两曲线之间)
- Distinguish displacement (vector) from distance (scalar) on FRQs在自由作答题中区分位移(向量)与路程(标量)
鼎睿学苑 · Dingrui Scholars — AP Calculus AB/BC Unit 9 Notes