IB Mathematics: Analysis & Approaches HL · 鼎睿学苑

Unit E4: Problem-Solving
Using Calculus
单元 E4:微积分的应用

The application layer. Where E1, E2, and E3 build the differentiation and integration machinery, E4 deploys it on word problems: optimisation, kinematics, area, volumes of revolution, and related rates. Every section follows the same four-step pattern: read the geometric or physical setup, write the function or relation, differentiate or integrate, and translate the result back into the problem's language.本单元是应用层。E1、E2、E3 搭好了微分与积分的机器,E4 用它们解应用题:最优化、运动学、面积、旋转体体积、相关变化率。每节都遵循同一四步法:读懂几何或物理情境、写出函数或关系式、求导或积分、再把结果翻译回题目语言。

IB AA HL · Topic 5.4 / 5.8 / 5.9 / 5.11 / 5.13 / 5.16 Papers 1 · 2 · 3 6 Concepts · SL + HL mix6 个核心概念 · SL + HL 混合

How to use this guide本指南使用说明

E4 is where calculus stops being an exercise in pattern matching and starts being a tool. Each section is organised by application type, not by technique. Pick the section that matches the question you face.E4 是微积分由"模式匹配练习"转为"工具"的阶段。各节按应用类型组织,不按技巧分。遇到题目,找对应小节即可。

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If you are cramming如果你在临阵磨枪

Memorise the kinematics chain: position $s(t)$, velocity $v = s'$, acceleration $a = v'$. Memorise the volume of revolution formula $V = \pi \int y^{2} \, dx$. Practise one optimisation problem (a box with maximum volume from a fixed sheet of card) end to end.

背熟运动学链:位置 $s(t)$、速度 $v = s'$、加速度 $a = v'$。背熟旋转体体积公式 $V = \pi \int y^{2} \, dx$。完整做一道最优化题(如固定面积纸板折盒求最大体积)。

If you are going for a 7如果你目标是 7 分

For optimisation, justify the maximum with the second-derivative test or a sign chart, not by inspection. For kinematics, master the distinction between displacement, distance, velocity, and speed. For volumes, do both $x$-axis ($\pi \int y^{2} dx$) and $y$-axis ($\pi \int x^{2} dy$) rotations.

最优化:用二阶导数检验或符号表正式验证极值,不要凭直观。运动学:分清位移与路程、速度与速率。体积:掌握绕 $x$ 轴($\pi \int y^{2} dx$)与绕 $y$ 轴($\pi \int x^{2} dy$)两种。

HL flagHL 标记说明 Related rates (E4.6) and $y$-axis volume integration (the second half of E4.5) are HL only. Optimisation, kinematics, area, and $x$-axis volumes are SL content that HL students inherit.相关变化率(E4.6)与绕 $y$ 轴的体积积分(E4.5 后半部分)为 HL 专属。最优化、运动学、面积、绕 $x$ 轴体积是 SL 内容,HL 学生继承。

Optimisation最优化 SL 5.8

Five steps for every optimisation problem.
  1. Identify the quantity to optimise. "Maximise the volume" or "minimise the surface area". Call this $Q$.
  2. Write $Q$ as a function of a single variable. If the problem has more than one variable, find a constraint equation that lets you eliminate all but one.
  3. Differentiate. Compute $\tfrac{dQ}{dx}$.
  4. Solve $\tfrac{dQ}{dx} = 0$. The critical points are the candidates for the optimum.
  5. Verify the optimum. Use the second-derivative test ($Q'' < 0$ for max, $Q'' > 0$ for min) or a sign chart of $Q'$. Check the boundary of the feasible region too if it is bounded.
The constraint equation is the easy step to forget. Two variables minus one constraint equals one degree of freedom, which is what you need.
最优化题的五步法。
  1. 识别待优化的量。"使体积最大"或"使表面积最小"。记为 $Q$。
  2. 把 $Q$ 写成单变量函数。若题目含多变量,找一个约束方程消去其余变量。
  3. 求导。算 $\tfrac{dQ}{dx}$。
  4. 解 $\tfrac{dQ}{dx} = 0$。临界点即极值候选。
  5. 验证。用二阶导数检验($Q'' < 0$ 为极大、$Q'' > 0$ 为极小)或一阶导符号表。若可行域有界,端点也要检查。
最易漏的一步是写约束方程。两个变量减一个约束等于一个自由度,正是求极值所需。
Worked Example E4.1 (box from a sheet)E4.1 例题(纸板折盒)

A rectangular sheet of card measures $24 \text{ cm}$ by $24 \text{ cm}$. Equal squares of side $x$ are cut from each corner and the sides folded up to make an open-top box. Find the value of $x$ that maximises the volume of the box, and state the maximum volume.一张 $24 \text{ cm} \times 24 \text{ cm}$ 的方形纸板,四角各裁掉边长为 $x$ 的小正方形,再把四边折起作成无盖纸盒。求使体积最大的 $x$,并写出最大体积。

Step 1. Quantity to optimise. Volume $V$ of the box.

第 1 步:待优化量。盒子的体积 $V$。

Step 2. Express $V$ as a function of $x$. The base is a square of side $24 - 2x$ and the height is $x$, so

第 2 步:把 $V$ 写成 $x$ 的函数。底面是边长 $24 - 2x$ 的正方形,高为 $x$,故

$$ V(x) \;=\; x \,(24 - 2x)^{2}, \qquad 0 < x < 12. $$

Step 3. Differentiate. Use the product rule and chain rule:

第 3 步:求导。乘积法则加链式法则:

$$ V'(x) \;=\; (24 - 2x)^{2} + x \cdot 2 (24 - 2x) \cdot (-2) \;=\; (24 - 2x)\bigl[(24 - 2x) - 4x\bigr] \;=\; (24 - 2x)(24 - 6x). $$

Step 4. Solve. $V'(x) = 0 \Rightarrow x = 12$ (rejected; gives zero volume) or $x = 4$.

第 4 步:求解。$V'(x) = 0 \Rightarrow x = 12$(舍去,体积为零)或 $x = 4$。

Step 5. Verify. Sign of $V'(x) = (24 - 2x)(24 - 6x)$ near $x = 4$: at $x = 3$, $V'(3) = 18 \cdot 6 = 108 > 0$; at $x = 5$, $V'(5) = 14 \cdot (-6) < 0$. So $V'$ changes from positive to negative at $x = 4$, confirming a local maximum.

第 5 步:验证。$V'(x) = (24 - 2x)(24 - 6x)$ 在 $x = 4$ 附近的符号:$x = 3$ 时 $V'(3) = 18 \cdot 6 = 108 > 0$;$x = 5$ 时 $V'(5) = 14 \cdot (-6) < 0$。符号由正变负,确为局部极大值。

Result. $V(4) = 4 \cdot 16^{2} = 4 \cdot 256 = 1024 \text{ cm}^{3}$. The maximum volume is $1024 \text{ cm}^{3}$, achieved when $x = 4 \text{ cm}$.

结果。$V(4) = 4 \cdot 16^{2} = 4 \cdot 256 = 1024 \text{ cm}^{3}$。最大体积为 $1024 \text{ cm}^{3}$,对应 $x = 4 \text{ cm}$。

Pitfall: the units and the domain陷阱:单位与定义域 Always state the domain of the variable you are optimising over ($0 < x < 12$ in the example) and include units in the final answer. Marks are deducted for "unitless" final answers in applied problems, and for declaring a maximum at a value outside the feasible domain.必须写出优化变量的定义域(例题中是 $0 < x < 12$),最终答案要带单位。应用题中无单位的最终答案要扣分;在可行域之外宣布极值同样扣分。
A rectangle is inscribed in a semicircle of radius $r$ with its base on the diameter. The rectangle that maximises area has width:在半径为 $r$ 的半圆中内接一矩形,底边在直径上。使矩形面积最大的宽为:
E4.1 · Q1
$r$
$r \sqrt{2}$
$2r$
$r / \sqrt{2}$
Place the semicircle at the origin. With half-width $x$, height is $\sqrt{r^{2} - x^{2}}$. Area $A = 2x \sqrt{r^{2} - x^{2}}$. Maximise $A^{2} = 4 x^{2}(r^{2} - x^{2})$ instead; $\tfrac{d}{dx}A^{2} = 8x r^{2} - 16 x^{3} = 0 \Rightarrow x^{2} = r^{2}/2 \Rightarrow x = r/\sqrt{2}$. Full width is $2x = r \sqrt{2}$.把半圆置于原点。设半宽 $x$,则高为 $\sqrt{r^{2} - x^{2}}$。面积 $A = 2x \sqrt{r^{2} - x^{2}}$。改优化 $A^{2} = 4 x^{2}(r^{2} - x^{2})$:$\tfrac{d}{dx}A^{2} = 8x r^{2} - 16 x^{3} = 0 \Rightarrow x^{2} = r^{2}/2 \Rightarrow x = r/\sqrt{2}$。全宽 $2x = r \sqrt{2}$。
Set up the area as $A = 2x \sqrt{r^{2} - x^{2}}$ where $x$ is the half-width. Optimising $A^{2}$ (monotone increasing in $A$) avoids the square root. The maximum is at $x = r/\sqrt{2}$, giving full width $r\sqrt{2}$.面积 $A = 2x \sqrt{r^{2} - x^{2}}$($x$ 为半宽)。优化 $A^{2}$(与 $A$ 同序)可避开根号。$x = r/\sqrt{2}$ 给最优,全宽 $r\sqrt{2}$。

Kinematics by Differentiation运动学:由位置求速度与加速度 SL 5.9

The kinematics chain. For a particle moving along a straight line with position $s(t)$ at time $t$: $$ \text{velocity} \;\; v(t) \;=\; \frac{ds}{dt} \;=\; s'(t), \qquad \text{acceleration} \;\; a(t) \;=\; \frac{dv}{dt} \;=\; v'(t) \;=\; s''(t). $$ Vocabulary.
  • Displacement is signed: $s(t_{2}) - s(t_{1})$.
  • Distance travelled over $[t_{1}, t_{2}]$ is $\int_{t_{1}}^{t_{2}} |v(t)| \, dt$ (which requires splitting where $v$ changes sign).
  • Velocity is signed (direction matters); speed is $|v|$.
  • At a change of direction, $v(t) = 0$. At a momentary rest, also $v(t) = 0$ but the particle may not change direction (need $v$ sign change to confirm).
运动学链。直线运动质点位置为 $s(t)$ 时: $$ \text{速度} \;\; v(t) \;=\; \frac{ds}{dt} \;=\; s'(t), \qquad \text{加速度} \;\; a(t) \;=\; \frac{dv}{dt} \;=\; v'(t) \;=\; s''(t). $$ 术语。
  • 位移(displacement是带符号的:$s(t_{2}) - s(t_{1})$。
  • $[t_{1}, t_{2}]$ 上的路程(distance travelled是 $\int_{t_{1}}^{t_{2}} |v(t)| \, dt$(需在 $v$ 变号处分段)。
  • 速度带符号(方向有意义);速率是 $|v|$。
  • 变向对应 $v(t) = 0$。瞬时静止也是 $v(t) = 0$,但未必变向(需用 $v$ 变号来判断)。
Worked Example E4.2 (particle on a line)E4.2 例题(直线运动质点)

A particle moves along a straight line with position $s(t) = t^{3} - 6 t^{2} + 9 t + 1$ for $t \ge 0$, where $s$ is in metres and $t$ in seconds. Find the times at which the particle is at rest, and determine whether the particle changes direction at each such time.一质点沿直线运动,位置 $s(t) = t^{3} - 6 t^{2} + 9 t + 1$($t \ge 0$,$s$ 以米计、$t$ 以秒计)。求质点瞬时静止的时刻,并判断每个时刻是否变向。

Velocity. $v(t) = s'(t) = 3 t^{2} - 12 t + 9 = 3 (t - 1)(t - 3)$.

速度。$v(t) = s'(t) = 3 t^{2} - 12 t + 9 = 3 (t - 1)(t - 3)$。

Times at rest. $v(t) = 0 \Rightarrow t = 1$ or $t = 3$.

静止时刻。$v(t) = 0 \Rightarrow t = 1$ 或 $t = 3$。

Direction change check. Sign of $v$:

变向检验。$v$ 的符号:

$t$$0 \le t < 1$$1 < t < 3$$t > 3$
$v(t)$$+$$-$$+$

Sign changes at both $t = 1$ ($+$ to $-$) and $t = 3$ ($-$ to $+$). The particle changes direction at both times.

$t = 1$(由 $+$ 转 $-$)与 $t = 3$(由 $-$ 转 $+$)两个时刻都变号。质点在个时刻都变向。

Acceleration. $a(t) = v'(t) = 6t - 12$, so $a(1) = -6 \text{ m/s}^{2}$ and $a(3) = +6 \text{ m/s}^{2}$ at the two turning points.

加速度。$a(t) = v'(t) = 6t - 12$,故 $a(1) = -6 \text{ m/s}^{2}$、$a(3) = +6 \text{ m/s}^{2}$。

A particle has velocity $v(t) = t^{2} - 4$ (m/s). Its acceleration at $t = 3$ s is:质点速度 $v(t) = t^{2} - 4$(m/s)。$t = 3$ s 时的加速度为:
E4.2 · Q1
$5 \text{ m/s}^{2}$
$6 \text{ m/s}^{2}$
$9 \text{ m/s}^{2}$
$0$
$a(t) = v'(t) = 2t$. At $t = 3$: $a = 6 \text{ m/s}^{2}$.$a(t) = v'(t) = 2t$。$t = 3$ 时 $a = 6 \text{ m/s}^{2}$。
Acceleration is the derivative of velocity. $v'(t) = 2t$, and at $t = 3$ this is $6$.加速度即速度的导数。$v'(t) = 2t$,$t = 3$ 时为 $6$。

Kinematics by Integration运动学:由速度积分求位置 SL 5.9

Run the kinematics chain backwards. $$ v(t) \;=\; \int a(t) \, dt + C_{1}, \qquad s(t) \;=\; \int v(t) \, dt + C_{2}. $$ The constants $C_{1}, C_{2}$ are fixed by initial conditions (typical: $v(0)$ and $s(0)$).

Two definite-integral applications.
  • Displacement from $t_{1}$ to $t_{2}$ is $\displaystyle\int_{t_{1}}^{t_{2}} v(t) \, dt$. Signed.
  • Distance travelled from $t_{1}$ to $t_{2}$ is $\displaystyle\int_{t_{1}}^{t_{2}} |v(t)| \, dt$. Always non-negative. Split the integral wherever $v$ changes sign.
反向运行运动学链。 $$ v(t) \;=\; \int a(t) \, dt + C_{1}, \qquad s(t) \;=\; \int v(t) \, dt + C_{2}. $$ 常数 $C_{1}, C_{2}$ 由初始条件确定(常用:$v(0)$ 与 $s(0)$)。

定积分的两类应用。
  • 位移($t_{1}$ 到 $t_{2}$):$\displaystyle\int_{t_{1}}^{t_{2}} v(t) \, dt$。带符号。
  • 路程($t_{1}$ 到 $t_{2}$):$\displaystyle\int_{t_{1}}^{t_{2}} |v(t)| \, dt$。非负。在 $v$ 变号处分段积分。
Worked Example E4.3 (displacement vs distance)E4.3 例题(位移与路程的区别)

A particle has velocity $v(t) = t^{2} - 4 t + 3$ (m/s) for $0 \le t \le 4$. Find (a) the displacement and (b) the total distance travelled over $[0, 4]$.质点速度 $v(t) = t^{2} - 4 t + 3$(m/s),$0 \le t \le 4$。求 (a) $[0, 4]$ 上的位移;(b) 总路程。

Factor $v$. $v(t) = (t - 1)(t - 3)$, so $v$ changes sign at $t = 1$ and $t = 3$.

分解 $v$。$v(t) = (t - 1)(t - 3)$,故 $v$ 在 $t = 1$ 与 $t = 3$ 处变号。

(a) Displacement.

(a) 位移。

$$ \int_{0}^{4} (t^{2} - 4t + 3) \, dt \;=\; \Bigl[ \tfrac{t^{3}}{3} - 2 t^{2} + 3t \Bigr]_{0}^{4} \;=\; \tfrac{64}{3} - 32 + 12 \;=\; \tfrac{64}{3} - 20 \;=\; \tfrac{4}{3} \text{ m}. $$

(b) Distance. Split at $t = 1$ and $t = 3$. On $[0, 1]$ and $[3, 4]$, $v \ge 0$; on $[1, 3]$, $v \le 0$.

(b) 路程。在 $t = 1$、$t = 3$ 处分段。$[0, 1]$ 与 $[3, 4]$ 上 $v \ge 0$,$[1, 3]$ 上 $v \le 0$。

$$ \int_{0}^{1} v \, dt \;=\; \tfrac{1}{3} - 2 + 3 \;=\; \tfrac{4}{3}, \qquad \int_{1}^{3} v \, dt \;=\; \Bigl( 9 - 18 + 9 \Bigr) - \Bigl( \tfrac{1}{3} - 2 + 3 \Bigr) \;=\; 0 - \tfrac{4}{3} \;=\; -\tfrac{4}{3}. $$ $$ \int_{3}^{4} v \, dt \;=\; \Bigl( \tfrac{64}{3} - 32 + 12 \Bigr) - \Bigl( 9 - 18 + 9 \Bigr) \;=\; \tfrac{4}{3} - 0 \;=\; \tfrac{4}{3}. $$

Total distance $= \tfrac{4}{3} + \bigl|-\tfrac{4}{3}\bigr| + \tfrac{4}{3} = \tfrac{12}{3} = 4 \text{ m}$.

总路程 $= \tfrac{4}{3} + \bigl|-\tfrac{4}{3}\bigr| + \tfrac{4}{3} = \tfrac{12}{3} = 4 \text{ m}$。

Cross-check. Displacement ($\tfrac{4}{3}$ m) does not equal distance ($4$ m), confirming the particle reversed direction on the way.

互相检验。位移($\tfrac{4}{3}$ m)$\ne$ 路程($4$ m),可知质点中途变向。

A particle starts at the origin with velocity $v(t) = 2t + 1$ (m/s). Its position at $t = 3$ s is:质点从原点出发,速度 $v(t) = 2t + 1$(m/s)。$t = 3$ s 时位置为:
E4.3 · Q1
$7 \text{ m}$
$10 \text{ m}$
$12 \text{ m}$
$9 \text{ m}$
$s(t) = \int (2t + 1) \, dt = t^{2} + t + C$. Initial condition $s(0) = 0$ gives $C = 0$. So $s(3) = 9 + 3 = 12 \text{ m}$.$s(t) = \int (2t + 1) \, dt = t^{2} + t + C$。初始条件 $s(0) = 0$ 给 $C = 0$。故 $s(3) = 9 + 3 = 12 \text{ m}$。
Integrate $v$ to get $s = t^{2} + t + C$. Use $s(0) = 0$ to find $C = 0$. Evaluate at $t = 3$.积 $v$ 得 $s = t^{2} + t + C$。由 $s(0) = 0$ 得 $C = 0$。在 $t = 3$ 处求值。

Area Between Curves曲线之间的面积 SL 5.11

Area between $y = f(x)$ and $y = g(x)$ over $[a, b]$ where $f(x) \ge g(x)$ throughout: $$ A \;=\; \int_{a}^{b} \bigl[ f(x) - g(x) \bigr] \, dx. $$ "Upper minus lower." The integrand is always non-negative under that assumption, so the result equals geometric area.

If the two curves cross, find the crossing points (solve $f(x) = g(x)$) and split the integral. On each piece, identify which curve is on top and integrate "upper minus lower" for that piece. Sum (or sum the absolute values) to get total geometric area.

Integration with respect to $y$ (HL preview, used in E4.5 for volumes around the $y$-axis): $$ A \;=\; \int_{c}^{d} \bigl[ x_{\text{right}}(y) - x_{\text{left}}(y) \bigr] \, dy. $$ Useful when the curves are easier to write as $x = $ function of $y$, or when the region is bounded by horizontal lines.
区间 $[a, b]$ 上 $y = f(x)$ 与 $y = g(x)$ 之间的面积(且 $f(x) \ge g(x)$ 全程成立): $$ A \;=\; \int_{a}^{b} \bigl[ f(x) - g(x) \bigr] \, dx. $$ 口诀:"上减下"。被积函数非负,结果等于几何面积。

若两曲线相交,先求交点(解 $f(x) = g(x)$),再分段积分。每段判断哪条在上,逐段"上减下"。各段相加(或取绝对值再加)得总几何面积。

对 $y$ 积分(HL 预习,E4.5 绕 $y$ 轴体积要用): $$ A \;=\; \int_{c}^{d} \bigl[ x_{\text{right}}(y) - x_{\text{left}}(y) \bigr] \, dy. $$ 适用于曲线写为 $x = $($y$ 的函数)更方便、或区域被水平直线界定时。
Worked Example E4.4 (parabola and line)E4.4 例题(抛物线与直线)

Find the area enclosed between $y = x^{2}$ and $y = 2x$.求 $y = x^{2}$ 与 $y = 2x$ 所围成的面积。

Intersection points. $x^{2} = 2x \Rightarrow x^{2} - 2x = 0 \Rightarrow x(x - 2) = 0$, so $x = 0$ and $x = 2$.

交点。$x^{2} = 2x \Rightarrow x(x - 2) = 0$,故 $x = 0$ 与 $x = 2$。

Identify the upper curve on $[0, 2]$. At $x = 1$: $y = x^{2} = 1$ vs $y = 2x = 2$, so the line $2x$ is above the parabola $x^{2}$.

判定 $[0, 2]$ 上的上方曲线。$x = 1$:$y = x^{2} = 1$,$y = 2x = 2$,故直线 $2x$ 在抛物线 $x^{2}$ 上方。

Integrate "upper minus lower".

"上减下"积分。

$$ A \;=\; \int_{0}^{2} (2x - x^{2}) \, dx \;=\; \Bigl[ x^{2} - \tfrac{x^{3}}{3} \Bigr]_{0}^{2} \;=\; 4 - \tfrac{8}{3} \;=\; \tfrac{4}{3}. $$
Area enclosed between $y = \sin x$ and $y = 0$ on $[0, \pi]$:$[0, \pi]$ 上 $y = \sin x$ 与 $y = 0$ 所围面积:
E4.4 · Q1
$2$
$\pi$
$0$
$1$
$\int_{0}^{\pi} \sin x \, dx = [-\cos x]_{0}^{\pi} = (-(-1)) - (-1) = 2$.$\int_{0}^{\pi} \sin x \, dx = [-\cos x]_{0}^{\pi} = 1 + 1 = 2$。
On $[0, \pi]$, $\sin x \ge 0$, so the integral is the geometric area, namely $\int_{0}^{\pi} \sin x \, dx = 2$.$[0, \pi]$ 上 $\sin x \ge 0$,积分即为几何面积 $\int_{0}^{\pi} \sin x \, dx = 2$。

Volumes of Revolution旋转体的体积 SL 5.11 · AHL 5.16

Rotation about the $x$-axis (SL). The region under $y = f(x)$ between $x = a$ and $x = b$, rotated $360^{\circ}$ about the $x$-axis, generates a solid of volume $$ V \;=\; \pi \int_{a}^{b} \bigl[ f(x) \bigr]^{2} \, dx \;=\; \pi \int_{a}^{b} y^{2} \, dx. $$ Rotation about the $y$-axis (HL). The region between $y = f(x)$ and the $y$-axis between $y = c$ and $y = d$, rotated about the $y$-axis, has volume $$ V \;=\; \pi \int_{c}^{d} \bigl[ g(y) \bigr]^{2} \, dy \;=\; \pi \int_{c}^{d} x^{2} \, dy, $$ where $x = g(y)$ is $y = f(x)$ solved for $x$.

Geometric origin (the "disk method"). Slice the solid into thin disks of thickness $dx$ (or $dy$), each disk approximately a cylinder of radius $y$ (or $x$). Volume of one disk $\approx \pi y^{2} \, dx$. Summing over all disks and taking the limit gives the integral.
绕 $x$ 轴旋转(SL)。$y = f(x)$ 下方、$x = a$ 到 $x = b$ 之间的区域绕 $x$ 轴旋转 $360^{\circ}$,生成立体的体积 $$ V \;=\; \pi \int_{a}^{b} \bigl[ f(x) \bigr]^{2} \, dx \;=\; \pi \int_{a}^{b} y^{2} \, dx. $$ 绕 $y$ 轴旋转(HL)。$y = f(x)$ 与 $y$ 轴之间、$y = c$ 到 $y = d$ 之间的区域绕 $y$ 轴旋转,体积为 $$ V \;=\; \pi \int_{c}^{d} \bigl[ g(y) \bigr]^{2} \, dy \;=\; \pi \int_{c}^{d} x^{2} \, dy, $$ 其中 $x = g(y)$ 是 $y = f(x)$ 对 $x$ 解出的形式。

几何来源("圆盘法")。把立体切成厚度 $dx$(或 $dy$)的薄圆盘,每片近似为半径 $y$(或 $x$)的圆柱。单片体积 $\approx \pi y^{2} \, dx$。求和取极限即得积分。
Worked Example E4.5a ($x$-axis rotation)E4.5a 例题(绕 $x$ 轴)

The region bounded by $y = \sqrt{x}$, the $x$-axis, and the lines $x = 0$ and $x = 4$ is rotated $360^{\circ}$ about the $x$-axis. Find the volume of the resulting solid.由 $y = \sqrt{x}$、$x$ 轴及 $x = 0$、$x = 4$ 围成的区域绕 $x$ 轴旋转 $360^{\circ}$,求所得立体的体积。

Apply the formula.

套用公式。

$$ V \;=\; \pi \int_{0}^{4} (\sqrt{x})^{2} \, dx \;=\; \pi \int_{0}^{4} x \, dx \;=\; \pi \Bigl[ \tfrac{x^{2}}{2} \Bigr]_{0}^{4} \;=\; \pi \cdot 8 \;=\; 8 \pi. $$

The volume is $8 \pi$ cubic units.

体积为 $8 \pi$ 立方单位。

Worked Example E4.5b ($y$-axis rotation) HLE4.5b 例题(绕 $y$ 轴)HL

The region bounded by $y = x^{2}$, the $y$-axis, and the line $y = 4$ is rotated $360^{\circ}$ about the $y$-axis. Find the volume.由 $y = x^{2}$、$y$ 轴及 $y = 4$ 围成的区域绕 $y$ 轴旋转 $360^{\circ}$。求体积。

Express $x$ in terms of $y$. $y = x^{2} \Rightarrow x = \sqrt{y}$ (taking the positive branch, since the region is in the first quadrant).

把 $x$ 表为 $y$ 的函数。$y = x^{2} \Rightarrow x = \sqrt{y}$(区域在第一象限,取正根)。

Identify the $y$-limits. The region runs from $y = 0$ to $y = 4$.

确定 $y$ 的积分限。$y$ 从 $0$ 到 $4$。

Apply the formula.

套用公式。

$$ V \;=\; \pi \int_{0}^{4} (\sqrt{y})^{2} \, dy \;=\; \pi \int_{0}^{4} y \, dy \;=\; \pi \Bigl[ \tfrac{y^{2}}{2} \Bigr]_{0}^{4} \;=\; 8 \pi. $$

The volume is $8 \pi$ cubic units. Note that this happens to equal the $x$-axis volume in E4.5a; this coincidence is not general.

体积为 $8 \pi$ 立方单位。本题数值恰巧与 E4.5a 绕 $x$ 轴的体积一致,纯属巧合,并非一般规律。

The region under $y = x$ from $x = 0$ to $x = 2$ is rotated about the $x$-axis. The volume is:$x = 0$ 到 $x = 2$ 之间 $y = x$ 下的区域绕 $x$ 轴旋转,体积为:
E4.5 · Q1
$2 \pi$
$4 \pi$
$\dfrac{8 \pi}{3}$
$8 \pi$
$V = \pi \int_{0}^{2} x^{2} \, dx = \pi \cdot \tfrac{8}{3} = \tfrac{8 \pi}{3}$. Geometrically, this is the cone of radius $2$ and height $2$, with formula $\tfrac{1}{3} \pi r^{2} h = \tfrac{1}{3} \pi \cdot 4 \cdot 2 = \tfrac{8 \pi}{3}$. The two methods agree.$V = \pi \int_{0}^{2} x^{2} \, dx = \pi \cdot \tfrac{8}{3} = \tfrac{8 \pi}{3}$。几何上是半径 $2$、高 $2$ 的圆锥,公式 $\tfrac{1}{3} \pi r^{2} h = \tfrac{1}{3} \pi \cdot 4 \cdot 2 = \tfrac{8 \pi}{3}$。两种方法一致。
$V = \pi \int y^{2} \, dx = \pi \int_{0}^{2} x^{2} \, dx = \tfrac{8 \pi}{3}$. This is the volume of a cone, which makes sense geometrically.$V = \pi \int y^{2} \, dx = \pi \int_{0}^{2} x^{2} \, dx = \tfrac{8 \pi}{3}$。几何上是圆锥体积,结果合理。

Related Rates相关变化率 HL AHL 5.13

The setup. Two or more quantities depend on time $t$, and they are connected by a geometric or physical relation. Given the rate at which one quantity changes, find the rate at which another changes at a specific moment.

Four-step method.
  1. Write down the relation connecting the quantities. For instance, $V = \tfrac{4}{3} \pi r^{3}$ for a sphere.
  2. Differentiate both sides with respect to $t$. Each variable picks up a $\tfrac{d \cdot}{dt}$ factor by the chain rule.
  3. Substitute the given rates and current values. Plug in numerical values after differentiating, not before. A rate that is given at a specific instant cannot be used until both sides are differentiated.
  4. Solve for the unknown rate.
情境。两个或更多量都依赖时间 $t$,并由几何或物理关系联系。已知其中一个量的变化率,求另一个量在某时刻的变化率。

四步法。
  1. 写出关系式。如球:$V = \tfrac{4}{3} \pi r^{3}$。
  2. 两边对 $t$ 求导。每个变量都按链式法则带上 $\tfrac{d \cdot}{dt}$ 因子。
  3. 代入给定变化率与当前值。必须在求导之后代入数值,不能之前代。某时刻的瞬时率必须留到两边求导完才能用。
  4. 解出待求变化率。
Worked Example E4.6 (balloon inflating)E4.6 例题(气球充气)

Air is pumped into a spherical balloon at a constant rate of $50 \text{ cm}^{3}/\text{s}$. Find the rate at which the radius is increasing at the moment when the radius is $5 \text{ cm}$.向球形气球以恒定速率 $50 \text{ cm}^{3}/\text{s}$ 充气。求气球半径为 $5 \text{ cm}$ 时半径的增长率。

Step 1. Relation. $V = \tfrac{4}{3} \pi r^{3}$.

第 1 步:关系式。$V = \tfrac{4}{3} \pi r^{3}$。

Step 2. Differentiate both sides with respect to $t$.

第 2 步:对 $t$ 求导。

$$ \frac{dV}{dt} \;=\; 4 \pi r^{2} \cdot \frac{dr}{dt}. $$

Step 3. Substitute. Given $\tfrac{dV}{dt} = 50$ and $r = 5$:

第 3 步:代入。已知 $\tfrac{dV}{dt} = 50$、$r = 5$:

$$ 50 \;=\; 4 \pi (5)^{2} \cdot \frac{dr}{dt} \;=\; 100 \pi \cdot \frac{dr}{dt}. $$

Step 4. Solve.

第 4 步:求解。

$$ \frac{dr}{dt} \;=\; \frac{50}{100 \pi} \;=\; \frac{1}{2 \pi} \;\approx\; 0.159 \text{ cm/s}. $$

The radius is increasing at about $0.16 \text{ cm/s}$ when $r = 5 \text{ cm}$.

$r = 5 \text{ cm}$ 时半径约以 $0.16 \text{ cm/s}$ 增长。

Pitfall: substituting too early陷阱:过早代入 If you plug $r = 5$ into $V = \tfrac{4}{3} \pi r^{3}$ before differentiating, you get $V = \tfrac{500 \pi}{3}$, which is a number with no $r$ in sight. Differentiating a constant gives zero, so $\tfrac{dV}{dt} = 0$ and the chain rule link to $\tfrac{dr}{dt}$ is lost. The "specific instant" values can only be used after the relation is differentiated symbolically. This is the single most common error on related-rates problems.若在求导前把 $r = 5$ 代入 $V = \tfrac{4}{3} \pi r^{3}$,得到 $V = \tfrac{500 \pi}{3}$(一个常数),已经没有 $r$。对常数求导为零,故 $\tfrac{dV}{dt} = 0$,与 $\tfrac{dr}{dt}$ 的链式联系丢失。"某时刻"的数值只能在符号求导之后代入。这是相关变化率题最常见的错误。
A square's area is increasing at $8 \text{ cm}^{2}/\text{s}$. The rate at which the side length is increasing when the side is $4 \text{ cm}$ is:正方形面积以 $8 \text{ cm}^{2}/\text{s}$ 增长。边长为 $4 \text{ cm}$ 时边长的增长率为:
E4.6 · Q1
$1 \text{ cm/s}$
$2 \text{ cm/s}$
$4 \text{ cm/s}$
$8 \text{ cm/s}$
$A = s^{2}$, so $\tfrac{dA}{dt} = 2 s \tfrac{ds}{dt}$. With $\tfrac{dA}{dt} = 8$ and $s = 4$: $8 = 8 \tfrac{ds}{dt}$, giving $\tfrac{ds}{dt} = 1 \text{ cm/s}$.$A = s^{2}$,故 $\tfrac{dA}{dt} = 2 s \tfrac{ds}{dt}$。$\tfrac{dA}{dt} = 8$、$s = 4$:$8 = 8 \tfrac{ds}{dt}$,得 $\tfrac{ds}{dt} = 1 \text{ cm/s}$。
Differentiate $A = s^{2}$ implicitly: $\tfrac{dA}{dt} = 2 s \tfrac{ds}{dt}$. Substitute the given values and solve for $\tfrac{ds}{dt}$.隐式求导 $A = s^{2}$:$\tfrac{dA}{dt} = 2 s \tfrac{ds}{dt}$。代入给定值求 $\tfrac{ds}{dt}$。

Exam Strategy and Common Pitfalls考试策略与常见陷阱

Optimisation (Paper 1 / Paper 2)最优化(Paper 1 / Paper 2)
  • Draw the figure. The geometric setup is often half the marks; a labelled diagram earns the M1 even before any calculus.
  • 画图。几何情境往往占一半分数;带标注的图能在动微积分之前就拿到 M1。
  • Justify the maximum or minimum. Either second-derivative test or first-derivative sign chart. Stating "this is the max" without justification costs the A1.
  • 正式验证极值。二阶导检验或一阶导符号表。光说"此为极大"无验证要丢 A1。
Kinematics (Paper 1 / Paper 2)运动学(Paper 1 / Paper 2)
  • Read the question for "displacement" vs "distance". The first wants the signed integral; the second wants the absolute-value integral with sign-change splitting.
  • 看题分清"位移"与"路程"。前者是带符号积分,后者要带绝对值并在变号处分段。
  • Initial conditions fix $C$. When integrating to find $s$ or $v$, write the $+ C$ explicitly and then use the initial value to solve for $C$.
  • 初始条件定 $C$。积分求 $s$ 或 $v$ 时显式写 $+ C$,再用初值解出 $C$。
Volumes and related rates (Paper 2 / Paper 3 HL)体积与相关变化率(Paper 2 / Paper 3 HL)
  • $\pi$ goes outside the integral. $V = \pi \int y^{2} \, dx$. Forgetting the $\pi$ is the canonical volume-of-revolution slip.
  • $\pi$ 写在积分号外。$V = \pi \int y^{2} \, dx$。漏写 $\pi$ 是绕轴体积题的标志性失误。
  • For $y$-axis rotation, square the $x$-expression (the radius from the axis), not the $y$-expression. The radius is always perpendicular to the axis of rotation.
  • 绕 $y$ 轴时平方的是 $x$ 表达式(到旋转轴的距离),不是 $y$ 表达式。"半径"总是与旋转轴垂直。
  • For related rates, differentiate first, substitute second. Never the other way round.
  • 相关变化率:先求导,再代值。顺序不可颠倒。

Flashcards闪卡

0 / 12 flipped已翻 0 / 12
Optimisation: 5 steps?最优化五步?
Identify $Q$, single-variable, differentiate, solve $Q' = 0$, verify.识别 $Q$,化单变量,求导,解 $Q' = 0$,验证。
Position to velocity?位置到速度?
$$v = \frac{ds}{dt}$$
Velocity to acceleration?速度到加速度?
$$a = \frac{dv}{dt} = \frac{d^{2} s}{dt^{2}}$$
Displacement from velocity?由速度求位移?
$$\int_{t_{1}}^{t_{2}} v(t) \, dt$$
Distance from velocity?由速度求路程?
$$\int_{t_{1}}^{t_{2}} |v(t)| \, dt$$Split at sign changes.在变号处分段。
Area between $f$ (upper) and $g$ on $[a, b]$?$[a, b]$ 上 $f$(上方)与 $g$ 之间的面积?
$$\int_{a}^{b} [f(x) - g(x)] \, dx$$
Volume rotating $y = f(x)$ about $x$-axis?$y = f(x)$ 绕 $x$ 轴旋转体积?
$$\pi \int_{a}^{b} y^{2} \, dx$$
Volume rotating about $y$-axis (HL)?绕 $y$ 轴旋转体积(HL)?
$$\pi \int_{c}^{d} x^{2} \, dy$$
Sphere volume formula?球的体积公式?
$$V = \tfrac{4}{3} \pi r^{3}$$
Related rates: first move?相关变化率:首要动作?
Differentiate the relation with respect to $t$ before substituting numerical values.先对 $t$ 求导关系式,再代入数值。
Justifying a maximum in optimisation?最优化中如何验证极大?
Second-derivative test ($Q'' < 0$) or sign chart of $Q'$.二阶导数检验($Q'' < 0$)或 $Q'$ 的符号表。
Particle changes direction at $t = t_{0}$ iff?质点在 $t = t_{0}$ 变向当且仅当?
$v(t_{0}) = 0$ and $v$ changes sign at $t_{0}$.$v(t_{0}) = 0$ $v$ 在 $t_{0}$ 变号。

Unit E4 Practice Quiz单元 E4 练习测验

A farmer has $40$ m of fence to enclose a rectangular pen against an existing wall (only three sides need fencing). The maximum area is:一农户有 $40$ m 围栏,要在已有的墙边围出矩形畜栏(只需围三面)。最大面积为:
Q1
$100 \text{ m}^{2}$
$200 \text{ m}^{2}$
$400 \text{ m}^{2}$
$300 \text{ m}^{2}$
Let width $w$ and length $\ell$. Fence: $\ell + 2 w = 40$, so $\ell = 40 - 2w$. Area $A = w (40 - 2 w) = 40 w - 2 w^{2}$. $A'(w) = 40 - 4 w = 0 \Rightarrow w = 10$. $A(10) = 10 \cdot 20 = 200 \text{ m}^{2}$.设宽 $w$、长 $\ell$。围栏:$\ell + 2 w = 40$,故 $\ell = 40 - 2w$。面积 $A = w (40 - 2 w) = 40 w - 2 w^{2}$。$A'(w) = 40 - 4 w = 0 \Rightarrow w = 10$。$A(10) = 10 \cdot 20 = 200 \text{ m}^{2}$。
Three sides of fencing: $\ell + 2w = 40$. Area $w(40 - 2w)$, derivative zero at $w = 10$. Length is then $20$, area $200 \text{ m}^{2}$.三面围栏:$\ell + 2w = 40$。面积 $w(40 - 2w)$,导数零点 $w = 10$。长 $20$,面积 $200 \text{ m}^{2}$。
A particle's velocity is $v(t) = 3 t^{2} - 6 t$ (m/s). The total distance travelled over $[0, 3]$ is:质点速度 $v(t) = 3 t^{2} - 6 t$(m/s)。$[0, 3]$ 上的总路程为:
Q2
$0 \text{ m}$
$9 \text{ m}$
$8 \text{ m}$
$4 \text{ m}$
$v(t) = 3t(t - 2)$, sign change at $t = 2$. On $[0, 2]$: $v \le 0$, so $\int_{0}^{2} v \, dt = [t^{3} - 3 t^{2}]_{0}^{2} = 8 - 12 = -4$. On $[2, 3]$: $v \ge 0$, $\int_{2}^{3} v \, dt = [t^{3} - 3 t^{2}]_{2}^{3} = (27 - 27) - (-4) = 4$. Distance $= 4 + 4 = 8 \text{ m}$.$v(t) = 3t(t - 2)$,$t = 2$ 处变号。$[0, 2]$ 上 $v \le 0$,$\int_{0}^{2} v \, dt = [t^{3} - 3 t^{2}]_{0}^{2} = -4$。$[2, 3]$ 上 $v \ge 0$,$\int_{2}^{3} v \, dt = (27 - 27) - (-4) = 4$。路程 $= 4 + 4 = 8 \text{ m}$。
Distance needs $|v|$. Split at the zero $t = 2$. On $[0, 2]$ the integral of $v$ is $-4$; take absolute value to get $4$. On $[2, 3]$ integral is $+4$. Total $8 \text{ m}$.路程要用 $|v|$。在零点 $t = 2$ 处分段。$[0, 2]$ 段 $v$ 积分为 $-4$,取绝对值 $4$。$[2, 3]$ 段为 $+4$。共 $8 \text{ m}$。
Area enclosed between $y = x^{3}$ and $y = x$ over $[0, 1]$:$[0, 1]$ 上 $y = x^{3}$ 与 $y = x$ 所围面积:
Q3
$\dfrac{1}{2}$
$\dfrac{1}{12}$
$\dfrac{1}{4}$
$\dfrac{1}{8}$
On $[0, 1]$, $x \ge x^{3}$. $\int_{0}^{1} (x - x^{3}) \, dx = [\tfrac{x^{2}}{2} - \tfrac{x^{4}}{4}]_{0}^{1} = \tfrac{1}{2} - \tfrac{1}{4} = \tfrac{1}{4}$.$[0, 1]$ 上 $x \ge x^{3}$。$\int_{0}^{1} (x - x^{3}) \, dx = [\tfrac{x^{2}}{2} - \tfrac{x^{4}}{4}]_{0}^{1} = \tfrac{1}{2} - \tfrac{1}{4} = \tfrac{1}{4}$。
Line $y = x$ is above $y = x^{3}$ on $[0, 1]$. Integrate "upper minus lower" to get $\tfrac{1}{4}$.$[0, 1]$ 上直线 $y = x$ 高于 $y = x^{3}$。"上减下"积分得 $\tfrac{1}{4}$。
The region under $y = e^{x}$ from $x = 0$ to $x = 1$ is rotated about the $x$-axis. The volume is:$x = 0$ 到 $x = 1$ 之间 $y = e^{x}$ 下的区域绕 $x$ 轴旋转,体积为:
Q4
$\pi (e - 1)$
$\dfrac{\pi (e^{2} - 1)}{2}$
$\dfrac{\pi (e^{2} - 1)}{2}$
$\pi e^{2}$
$V = \pi \int_{0}^{1} (e^{x})^{2} \, dx = \pi \int_{0}^{1} e^{2x} \, dx = \pi \bigl[ \tfrac{e^{2x}}{2} \bigr]_{0}^{1} = \tfrac{\pi (e^{2} - 1)}{2}$.$V = \pi \int_{0}^{1} (e^{x})^{2} \, dx = \pi \int_{0}^{1} e^{2x} \, dx = \pi \bigl[ \tfrac{e^{2x}}{2} \bigr]_{0}^{1} = \tfrac{\pi (e^{2} - 1)}{2}$。
Square $e^{x}$ to get $e^{2x}$, integrate, multiply by $\pi$. Result: $\tfrac{\pi (e^{2} - 1)}{2}$.把 $e^{x}$ 平方得 $e^{2x}$,积分,乘 $\pi$。结果:$\tfrac{\pi (e^{2} - 1)}{2}$。
A conical tank has its vertex pointing down and is being filled with water at $2 \text{ m}^{3}/\text{min}$. The cone has height equal to twice its base radius ($h = 2 r$). Find $\tfrac{dh}{dt}$ when $h = 4 \text{ m}$.一倒置圆锥水箱以 $2 \text{ m}^{3}/\text{min}$ 注水。圆锥高为底半径的两倍($h = 2 r$)。求 $h = 4 \text{ m}$ 时 $\tfrac{dh}{dt}$。
Q5
$\dfrac{1}{\pi}$ m/min
$\dfrac{2}{\pi}$ m/min
$\dfrac{1}{2 \pi}$ m/min
$\pi$ m/min
Cone: $V = \tfrac{1}{3} \pi r^{2} h$. Substitute $r = h/2$: $V = \tfrac{1}{3} \pi (h/2)^{2} h = \tfrac{\pi h^{3}}{12}$. Differentiate: $\tfrac{dV}{dt} = \tfrac{\pi h^{2}}{4} \tfrac{dh}{dt}$. With $\tfrac{dV}{dt} = 2$, $h = 4$: $2 = \tfrac{\pi \cdot 16}{4} \tfrac{dh}{dt} = 4 \pi \tfrac{dh}{dt}$, so $\tfrac{dh}{dt} = \tfrac{1}{2 \pi}$. Wait, let me recompute. Actually: $\tfrac{\pi h^{2}}{4}$ at $h = 4$ gives $\tfrac{16 \pi}{4} = 4 \pi$. So $\tfrac{dh}{dt} = \tfrac{2}{4 \pi} = \tfrac{1}{2 \pi}$. Hmm, that matches option 2, not 1. Let me re-examine: $\tfrac{d}{dh}(\tfrac{\pi h^{3}}{12}) = \tfrac{\pi h^{2}}{4}$. Yes. So $\tfrac{dh}{dt} = \tfrac{2}{\pi h^{2}/4} = \tfrac{8}{\pi h^{2}}$. At $h = 4$: $\tfrac{8}{16 \pi} = \tfrac{1}{2\pi}$ m/min, which is option 2.圆锥:$V = \tfrac{1}{3} \pi r^{2} h$。代 $r = h/2$:$V = \tfrac{\pi h^{3}}{12}$。求导:$\tfrac{dV}{dt} = \tfrac{\pi h^{2}}{4} \tfrac{dh}{dt}$。$h = 4$ 时,$\tfrac{\pi \cdot 16}{4} = 4 \pi$,故 $\tfrac{dh}{dt} = \tfrac{2}{4 \pi} = \tfrac{1}{2 \pi}$ m/min。
Express $V$ in $h$ alone using the constraint $r = h/2$. Differentiate implicitly with respect to $t$, then substitute. Be careful with the $h^{2}$ coefficient.用约束 $r = h/2$ 把 $V$ 表为单 $h$ 函数。对 $t$ 隐式求导,再代入。注意 $h^{2}$ 系数。

Readiness Checklist备考清单

Tick each item when you can do it cold, without notes, on your first attempt.

每一条都要"裸做"做对(不看笔记、一次过)才打勾。

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