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考前總複習 期中 11/6

期中考帶進場的整理

Midterm Open-Note Sheet (Ch 1–3)

這不是第四份講義,是考前的濃縮版。三章的觀念在第 1–3 章已經推導過了,這裡只放考場上用得到的:英文公式表、判斷流程、英文答題句型,和 7 題要自己動筆算的練習。列印版 PDF 在桌面的「工程數學」資料夾。

課本小節
  • 老師例題總表(考上課教例)
  • 英文公式表(Ch 1–3)
  • 30 秒判斷題型
  • 考卷英文與答題句型
  • 最常扣分的 10 個地方
  • 練習題 7 題含詳解
⚠ 先看這個

這份整理怎麼用、剩下三週怎麼排

How to Use This Page
白話講

期中考是 11/6(週五),佔學期成績 30%(平時考 40%、期中 30%、期末 30%)。老師說題目用英文出、可以帶自己整理的資料,而且期中期末都考上課教的例題。所以這頁有兩個用途:

① 考前:照下面的進度一天一小段,把三章的觀念頁看過,老師的每一題例題都自己重算一次(下一段有總表)。② 考試當天:把公式表、判斷流程、英文句型印出來帶進去。

週次每天 45–60 分鐘,一週 5 天對應頁面
10/19–10/23Ch1:每天 2–3 個觀念(m1-1 ~ m1-13,1.6 正交軌跡跳過),每個觀念做完底下的英文考題第 1 章
10/26–10/30Ch2:每天 2 個觀念(m2-1 ~ m2-10),重點是 m2-4、m2-8、m2-9第 2 章
11/2–11/5Ch3(m3-1 ~ m3-6)→ 老師例題總表遮答案重算一輪 → 本頁練習題 → 印出 PDF第 3 章、本頁

考試範圍要跟老師確認。學校教學大綱寫的期中範圍是「課程簡介、一階、二階」;老師目前給了第 1–3 章的投影片。保險起見三章都準備,第三章規則跟第二章幾乎一樣,多花的時間不多。

帶資料進場不代表可以不練。考場上沒有時間現學——公式表是拿來「確認」的,不是拿來「學」的。題型判斷和計算一定要考前就熟。

列印版:公式表、題型判斷、考卷英文、答題句型已排成 A4 的 PDF,放在桌面「工程數學」資料夾:工數期中_帶進場整理.pdf。

⚠ 期中必考

老師上課的例題總表(期中期末都考上課教例)

Teacher's Worked Examples
白話講

老師說期中、期末都考上課教的例題。所以最有效的準備不是做新題目,而是把下面每一題自己從頭算一次,算到不看詳解也能寫出來。

每題的完整推導都在講堂對應的觀念裡(最右欄),這張表只放題目、方法和最後答案——考試時拿來對答案,也印在帶進場的 PDF 裡。1.6 正交軌跡的 Ex.17、Ex.18 期中跳過,沒有列。

第 1 章

y′=3y, y(0)=5.7y' = 3y,\ y(0) = 5.7
方法 可分離答案 y=5.7e3xy = 5.7e^{3x}詳解 m1-2
Ex.1 畫 y′=xyy' = xy 的方向場
方法 等傾線答案 等傾線 xy=kxy = k(雙曲線)詳解 m1-3
Ex.2 9yy′+4x=09yy' + 4x = 0
方法 可分離答案 x29+y24=c\displaystyle \frac{x^2}{9} + \frac{y^2}{4} = c詳解 m1-4
Ex.3 y′=1+y2y' = 1 + y^2
方法 可分離答案 y=tan⁡(x+c)y = \tan(x + c)詳解 m1-4
Ex.4 y′+5x4y2=0, y(0)=1y' + 5x^4y^2 = 0,\ y(0) = 1
方法 可分離答案 y=1x5+1\displaystyle y = \frac{1}{x^5 + 1}詳解 m1-4
Ex.5 2xyy′=y2−x22xyy' = y^2 - x^2
方法 R-1:u=y/xu = y/x答案 x2+y2=cxx^2 + y^2 = cx詳解 m1-5
Ex.6 y′=yx+2x3cos⁡x2y, y(π)=0\displaystyle y' = \frac{y}{x} + \frac{2x^3\cos x^2}{y},\ y(\sqrt\pi) = 0
方法 R-1:u=y/xu = y/x答案 y=x2sin⁡x2y = x\sqrt{2\sin x^2}詳解 m1-5
Ex.7 y′=(2x+y−1x−2)2\displaystyle y' = \left(\frac{2x + y - 1}{x - 2}\right)^2
方法 R-2 Case 1:α=2, β=−3\alpha = 2,\ \beta = -3答案 27tan⁡−12Y+3X7X=ln⁡∣X∣+c\displaystyle \frac{2}{\sqrt7}\tan^{-1}\frac{2Y + 3X}{\sqrt7 X} = \ln|X| + c,X=x−2, Y=y+3X = x - 2,\ Y = y + 3詳解 m1-6
Ex.8 y′=2x+y−14x+2y−4\displaystyle y' = \frac{2x + y - 1}{4x + 2y - 4}
方法 R-2 Case 2:v=2x+y2v = \frac{2x + y}{2}答案 −x5+2y5−225ln⁡∣10x+5y−9∣=c\displaystyle -\frac x5 + \frac{2y}{5} - \frac{2}{25}\ln|10x + 5y - 9| = c詳解 m1-6
Ex.9 (x3+3xy2)dx+(3x2y+y3)dy=0(x^3 + 3xy^2)dx + (3x^2y + y^3)dy = 0
方法 正合答案 x4+6x2y2+y4=cx^4 + 6x^2y^2 + y^4 = c詳解 m1-7
Ex.10 sin⁡xcosh⁡y dx−cos⁡xsinh⁡y dy=0, y(0)=3\sin x\cosh y\,dx - \cos x\sinh y\,dy = 0,\ y(0) = 3
方法 正合答案 cos⁡xcosh⁡y=cosh⁡3\cos x\cosh y = \cosh 3詳解 m1-7
Ex.11 y dx−x dy=0y\,dx - x\,dy = 0
方法 積分因子 F=1x2F = \frac{1}{x^2}答案 y=cxy = cx詳解 m1-8
Ex.12 2sin⁡y2 dx+xycos⁡y2 dy=02\sin y^2\,dx + xy\cos y^2\,dy = 0
方法 積分因子 F=x3F = x^3答案 x4sin⁡y2=cx^4\sin y^2 = c詳解 m1-8
Ex.13 2xy dx+(4y+3x2)dy=0, y(0.2)=−1.52xy\,dx + (4y + 3x^2)dy = 0,\ y(0.2) = -1.5
方法 積分因子 F(y)=y2F(y) = y^2答案 x2y3+y4=4.9275x^2y^3 + y^4 = 4.9275詳解 m1-8
Ex.14 (2y2−9xy)dx+(3xy−6x2)dy=0(2y^2 - 9xy)dx + (3xy - 6x^2)dy = 0
方法 積分因子 F=xayb→xyF = x^ay^b \to xy答案 x2y3−3x3y2=cx^2y^3 - 3x^3y^2 = c詳解 m1-8
Ex.15 y′−y=e2xy' - y = e^{2x}
方法 一階線性答案 y=e2x+cexy = e^{2x} + ce^x詳解 m1-9
y′+2y=ex(3sin⁡2x+2cos⁡2x)y' + 2y = e^x(3\sin 2x + 2\cos 2x)
方法 一階線性答案 y=ce−2x+exsin⁡2xy = ce^{-2x} + e^x\sin 2x詳解 m1-9
Ex.16 y′−Ay=−By2y' - Ay = -By^2
方法 Bernoulli:u=y−1u = y^{-1}答案 y=1B/A+ce−Ax\displaystyle y = \frac{1}{B/A + ce^{-Ax}}詳解 m1-10

第 2 章

y′′−y=0, y(0)=4, y′(0)=−2y'' - y = 0,\ y(0) = 4,\ y'(0) = -2
方法 常係數(相異實根)答案 y=ex+3e−xy = e^x + 3e^{-x}詳解 m2-2
x2y′′−xy′+y=0x^2y'' - xy' + y = 0,已知 y1=xy_1 = x
方法 降階法答案 y2=xln⁡xy_2 = x\ln x詳解 m2-3
y′′+y′−2y=0, y(0)=4, y′(0)=−5y'' + y' - 2y = 0,\ y(0) = 4,\ y'(0) = -5
方法 相異實根答案 y=ex+3e−2xy = e^x + 3e^{-2x}詳解 m2-4
y′′+y′+0.25y=0, y(0)=3, y′(0)=−3.5y'' + y' + 0.25y = 0,\ y(0) = 3,\ y'(0) = -3.5
方法 重根答案 y=(3−2x)e−0.5xy = (3 - 2x)e^{-0.5x}詳解 m2-4
y′′+0.4y′+9.04y=0, y(0)=0, y′(0)=3y'' + 0.4y' + 9.04y = 0,\ y(0) = 0,\ y'(0) = 3
方法 複數根答案 y=e−0.2xsin⁡3xy = e^{-0.2x}\sin 3x詳解 m2-4
練習:y′′+2y′+5y=0, y(0)=1, y′(0)=5y'' + 2y' + 5y = 0,\ y(0) = 1,\ y'(0) = 5
方法 複數根答案 y=e−x(cos⁡2x+3sin⁡2x)y = e^{-x}(\cos 2x + 3\sin 2x)詳解 m2-4
練習:y′′+y=0, y(0)=3, y(π)=−3y'' + y = 0,\ y(0) = 3,\ y(\pi) = -3
方法 邊界值問題答案 y=3cos⁡x+c2sin⁡xy = 3\cos x + c_2\sin x(無限多解)詳解 m2-4
x2y′′+1.5xy′−0.5y=0x^2y'' + 1.5xy' - 0.5y = 0
方法 Euler–Cauchy(相異)答案 y=c1x+c2x\displaystyle y = c_1\sqrt x + \frac{c_2}{x}詳解 m2-5
x2y′′−5xy′+9y=0x^2y'' - 5xy' + 9y = 0
方法 Euler–Cauchy(重根)答案 y=(c1+c2ln⁡x)x3y = (c_1 + c_2\ln x)x^3詳解 m2-5
x2y′′+0.6xy′+16.04y=0x^2y'' + 0.6xy' + 16.04y = 0
方法 Euler–Cauchy(複數)答案 y=x0.2[c1cos⁡(4ln⁡x)+c2sin⁡(4ln⁡x)]y = x^{0.2}[c_1\cos(4\ln x) + c_2\sin(4\ln x)]詳解 m2-5
證明 WW 處處為 00 或處處不為 00
方法 W′+pW=0W' + pW = 0答案 W=ce−∫p dx\displaystyle W = ce^{-\int p\,dx}詳解 m2-6
y′′+4y=8x2y'' + 4y = 8x^2
方法 待定係數答案 yp=2x2−1y_p = 2x^2 - 1詳解 m2-8
y′′+3y′+2.25y=−10e−1.5x, y(0)=1, y′(0)=0y'' + 3y' + 2.25y = -10e^{-1.5x},\ y(0) = 1,\ y'(0) = 0
方法 待定係數+修正(乘 x2x^2)答案 y=(1+1.5x−5x2)e−1.5xy = (1 + 1.5x - 5x^2)e^{-1.5x}詳解 m2-8
y′′+2y′+0.75y=2cos⁡x−0.25sin⁡x+0.09xy'' + 2y' + 0.75y = 2\cos x - 0.25\sin x + 0.09x,y(0)=2.78, y′(0)=−0.43y(0) = 2.78,\ y'(0) = -0.43
方法 待定係數+加法規則答案 y=3.1e−x/2+sin⁡x+0.12x−0.32y = 3.1e^{-x/2} + \sin x + 0.12x - 0.32詳解 m2-8
y′′+y=sec⁡xy'' + y = \sec x
方法 參數變異答案 y=(c1+ln⁡∣cos⁡x∣)cos⁡x+(c2+x)sin⁡xy = (c_1 + \ln|\cos x|)\cos x + (c_2 + x)\sin x詳解 m2-9

第 3 章

y′′′−2y′′+2y′=0y''' - 2y'' + 2y' = 0
方法 特徵根 0, 1±i0,\ 1 \pm i答案 y=c1+ex(c2cos⁡x+c3sin⁡x)y = c_1 + e^x(c_2\cos x + c_3\sin x)詳解 m3-2
y(5)−3y(4)+3y′′′−y′′=0y^{(5)} - 3y^{(4)} + 3y''' - y'' = 0
方法 重根 λ2(λ−1)3\lambda^2(\lambda - 1)^3答案 y=c1+c2x+(c3+c4x+c5x2)exy = c_1 + c_2x + (c_3 + c_4x + c_5x^2)e^x詳解 m3-3
y′′′+3y′′+3y′+y=30e−xy''' + 3y'' + 3y' + y = 30e^{-x},y(0)=3, y′(0)=−3, y′′(0)=−47y(0) = 3,\ y'(0) = -3,\ y''(0) = -47
方法 待定係數(乘 x3x^3)答案 y=(3−25x2)e−x+5x3e−xy = (3 - 25x^2)e^{-x} + 5x^3e^{-x}詳解 m3-4
x3y′′′−3x2y′′+6xy′−6y=x4ln⁡xx^3y''' - 3x^2y'' + 6xy' - 6y = x^4\ln x
方法 三階 EC+參數變異答案 y=c1x+c2x2+c3x3+x46(ln⁡x−116)\displaystyle y = c_1x + c_2x^2 + c_3x^3 + \frac{x^4}{6}\left(\ln x - \frac{11}{6}\right)詳解 m3-5

怎麼用這張表:遮住「答案」欄,看題目先說出「方法」,再動筆算,最後才對答案。方法說不出來的,回到「詳解」那個觀念重看推導。

核心工具

公式表① Chapter 1 First-Order ODEs

Formula Sheet: Chapter 1
TypeFormMethod / Solution
Separableg(y) dy=f(x) dxg(y)\,dy = f(x)\,dx∫g dy=∫f dx+c\displaystyle \int g\,dy = \int f\,dx + c
R-1y′=g(y/x)y' = g(y/x)u=yx, y′=u+xu′, dug(u)−u=dxxu = \tfrac{y}{x},\ y' = u + xu',\ \tfrac{du}{g(u)-u} = \tfrac{dx}{x}
R-2, ae−bg≠0ae - bg \neq 0y′=f ⁣(ax+by+cgx+ey+h)y' = f\!\left(\tfrac{ax+by+c}{gx+ey+h}\right)x=X+α, y=Y+β;  aα+bβ+c=0, gα+eβ+h=0 → R-1x = X+\alpha,\ y = Y+\beta;\ \ a\alpha+b\beta+c = 0,\ g\alpha+e\beta+h = 0 \ \to\ \text{R-1}
R-2, ae−bg=0ae - bg = 0samev=ax+bya, dvdx=1+badydx → separablev = \tfrac{ax+by}{a},\ \tfrac{dv}{dx} = 1 + \tfrac{b}{a}\tfrac{dy}{dx} \ \to\ \text{separable}
ExactM dx+N dy=0, My=NxM\,dx + N\,dy = 0,\ M_y = N_xu=∫M dx+k(y), uy=N;  u(x,y)=c\displaystyle u = \int M\,dx + k(y),\ u_y = N;\ \ u(x,y) = c
Integrating factorMy≠NxM_y \neq N_xF(x)=e∫My−NxNdx  or  F(y)=e∫Nx−MyMdy\displaystyle F(x) = e^{\int \frac{M_y - N_x}{N}dx}\ \ \text{or}\ \ F(y) = e^{\int \frac{N_x - M_y}{M}dy}
Lineary′+p(x) y=r(x)y' + p(x)\,y = r(x)y=e−h[∫ehr dx+c], h=∫p dx\displaystyle y = e^{-h}\left[\int e^{h}r\,dx + c\right],\ h = \int p\,dx
Bernoulliy′+py=r yay' + py = r\,y^{a}u=y1−a: u′+(1−a)p u=(1−a)ru = y^{1-a}:\ u' + (1-a)p\,u = (1-a)r

先除成標準式:線性、Bernoulli 的 y′y' 係數要是 11。答案記得換回原變數(u→y/xu \to y/x、X→x−αX \to x - \alpha)。1.6 正交軌跡期中不考,沒有列。

核心工具

公式表② Chapter 2 Second-Order Linear ODEs

Formula Sheet: Chapter 2
TypeFormMethod / Solution
Const. coeff.y′′+ay′+by=0y'' + ay' + by = 0λ2+aλ+b=0\lambda^2 + a\lambda + b = 0
— distinct realλ1≠λ2\lambda_1 \neq \lambda_2y=c1eλ1x+c2eλ2xy = c_1e^{\lambda_1x} + c_2e^{\lambda_2x}
— double rootλ=−a/2\lambda = -a/2y=(c1+c2x) e−ax/2y = (c_1 + c_2x)\,e^{-ax/2}
— complexλ=−a2±iω\lambda = -\tfrac a2 \pm i\omegay=e−ax/2(c1cos⁡ωx+c2sin⁡ωx), ω=b−a2/4y = e^{-ax/2}(c_1\cos\omega x + c_2\sin\omega x),\ \omega = \sqrt{b - a^2/4}
Euler–Cauchyx2y′′+axy′+by=0x^2y'' + axy' + by = 0m2+(a−1)m+b=0m^2 + (a-1)m + b = 0
— distinct / doublec1xm1+c2xm2/(c1+c2ln⁡x) xmc_1x^{m_1} + c_2x^{m_2}\quad /\quad (c_1 + c_2\ln x)\,x^{m}
— complex μ±iν\mu \pm i\nuxμ[c1cos⁡(νln⁡x)+c2sin⁡(νln⁡x)]x^{\mu}\left[c_1\cos(\nu\ln x) + c_2\sin(\nu\ln x)\right]
Reduction of ordery1 knowny_1 \text{ known}y2=y1∫e−∫p dxy12 dx\displaystyle y_2 = y_1\int \frac{e^{-\int p\,dx}}{y_1^2}\,dx
WronskianW=y1y2′−y1′y2;  W≠0  ⟺  independent;  W=c e−∫p dx\displaystyle W = y_1y_2' - y_1'y_2;\ \ W \neq 0 \iff \text{independent};\ \ W = c\,e^{-\int p\,dx}
Nonhomogeneousy′′+py′+qy=ry'' + py' + qy = ry=yh+ypy = y_h + y_p
Undetermined coeff.eγx; xn; cos⁡ωx,sin⁡ωxe^{\gamma x};\ x^n;\ \cos\omega x, \sin\omega xCeγx; Knxn+⋯+K0; Kcos⁡ωx+Msin⁡ωxCe^{\gamma x};\ K_nx^n + \cdots + K_0;\ K\cos\omega x + M\sin\omega x
— modificationtrial in yh: ×x (simple root), ×x2 (double root)\text{trial in } y_h:\ \times x \text{ (simple root)},\ \times x^2 \text{ (double root)}
Variation of parametersyp=−y1∫y2rWdx+y2∫y1rWdx\displaystyle y_p = -y_1\int\frac{y_2r}{W}dx + y_2\int\frac{y_1r}{W}dx

Euler–Cauchy 的中間係數是 a−1a - 1。初始條件要代進 yh+ypy_h + y_p。

核心工具

公式表③ Chapter 3 + 常用積分

Formula Sheet: Chapter 3 & Integrals
TypeFormMethod / Solution
nn-th order const. coeff.y(n)+⋯+a0y=0y^{(n)} + \cdots + a_0y = 0λn+⋯+a1λ+a0=0\lambda^n + \cdots + a_1\lambda + a_0 = 0
— root of order mmeλx, xeλx, …, xm−1eλxe^{\lambda x},\ xe^{\lambda x},\ \ldots,\ x^{m-1}e^{\lambda x}
— complex v±iωv \pm i\omega, order mmxkevxcos⁡ωx, xkevxsin⁡ωx,  k=0,…,m−1x^k e^{vx}\cos\omega x,\ x^ke^{vx}\sin\omega x,\ \ k = 0, \ldots, m-1
Modification (order nn)trial is a root of order k⇒× xk\text{trial is a root of order } k \Rightarrow \times\,x^k
Variation of parametersyp=∑kyk∫WkW r dx,Wk: k-th column→(0,…,0,1)T\displaystyle y_p = \sum_k y_k\int\frac{W_k}{W}\,r\,dx,\quad W_k:\ k\text{-th column} \to (0,\ldots,0,1)^T
3×33\times3 determinanta(ei−fh)−b(di−fg)+c(dh−eg)a(ei - fh) - b(di - fg) + c(dh - eg)
常用積分 · Useful Integrals
∫f′f dx=ln⁡∣f∣+c\int\frac{f'}{f}\,dx = \ln|f| + c
∫dxa2+x2=1atan⁡−1xa+c\int\frac{dx}{a^2 + x^2} = \frac1a\tan^{-1}\frac xa + c
∫tan⁡x dx=−ln⁡∣cos⁡x∣+c\int\tan x\,dx = -\ln|\cos x| + c
∫sec⁡x dx=ln⁡∣sec⁡x+tan⁡x∣+c\int\sec x\,dx = \ln|\sec x + \tan x| + c
∫xnln⁡x dx=xn+1n+1ln⁡x−xn+1(n+1)2+c\int x^n\ln x\,dx = \frac{x^{n+1}}{n+1}\ln x - \frac{x^{n+1}}{(n+1)^2} + c∫xnln⁡x dx=xn+1n+1ln⁡x−xn+1(n+1)2+c\begin{aligned}&\int x^n\ln x\,dx \\[2pt] &\quad = \frac{x^{n+1}}{n+1}\ln x - \frac{x^{n+1}}{(n+1)^2} + c\end{aligned}
∫eaxsin⁡bx dx=eax(asin⁡bx−bcos⁡bx)a2+b2+c\int e^{ax}\sin bx\,dx = \frac{e^{ax}(a\sin bx - b\cos bx)}{a^2 + b^2} + c∫eaxsin⁡bx dx=eax(asin⁡bx−bcos⁡bx)a2+b2+c\begin{aligned}&\int e^{ax}\sin bx\,dx \\[2pt] &\quad = \frac{e^{ax}(a\sin bx - b\cos bx)}{a^2 + b^2} + c\end{aligned}
eiθ=cos⁡θ+isin⁡θ,cosh⁡x=ex+e−x2,sinh⁡x=ex−e−x2e^{i\theta} = \cos\theta + i\sin\theta,\quad \cosh x = \tfrac{e^x + e^{-x}}2,\quad \sinh x = \tfrac{e^x - e^{-x}}2eiθ=cos⁡θ+isin⁡θ,cosh⁡x=ex+e−x2,sinh⁡x=ex−e−x2\begin{aligned}&e^{i\theta} = \cos\theta + i\sin\theta, \\[2pt] &\cosh x = \tfrac{e^x + e^{-x}}2, \\[2pt] &\sinh x = \tfrac{e^x - e^{-x}}2\end{aligned}
考前必看

30 秒判斷題型

Which Method?
白話講

拿到題目先別急著算,先數階數,再照下面的順序一格一格問。

一階:依序問→ 方法
1分得開 xx 和 yy?Separable
2能寫成 y′+p(x) y=r(x)y' + p(x)\,y = r(x)?Linear 公式
3右邊多一個 yay^a?Bernoulli:u=y1−au = y^{1-a}
4M dx+N dyM\,dx + N\,dy,My=NxM_y = N_x?Exact
5My≠NxM_y \neq N_x積分因子 F(x)F(x) → F(y)F(y) → xaybx^ay^b
6只出現 y/xy/x?R-1:u=y/xu = y/x
7ax+by+cgx+ey+h\frac{ax+by+c}{gx+ey+h}?R-2:先算 ae−bgae - bg
二階/nn 階:依序問→ 方法
1係數是常數?特徵方程 λ2+aλ+b=0\lambda^2 + a\lambda + b = 0
2x2y′′+axy′+byx^2y'' + axy' + by?Euler–Cauchy:m2+(a−1)m+b=0m^2 + (a-1)m + b = 0
3係數是別的函數,但給了 y1y_1?降階法
4右邊 ≠0\neq 0,而且是 eγxe^{\gamma x}、多項式、sin⁡\sin、cos⁡\cos?待定係數(撞到 yhy_h 要乘 xx)
5右邊是 sec⁡x\sec x、tan⁡x\tan x、ln⁡x\ln x、1x\frac1x?參數變異
考前必看

考卷上的英文怎麼讀

Exam Vocabulary
白話講

題目的動詞決定你要交出什麼。看到 Solve 跟看到 Show that,要寫的東西完全不同。

英文意思你要交出的東西
Solve …求通解(沒給條件)答案要有任意常數
Solve the initial value problem (IVP)解初值問題求出常數,答案不能有 cc
boundary value problem (BVP)邊界值問題條件在兩個不同的點,可能無解或無限多解
Find the general solution求通解一階 1 個常數、二階 2 個
Find a particular solution求一個特解 ypy_p不用加 yhy_h
Show that … is a solution / Verify證明/驗證是解代進去,左右相等
Test for exactness / Show that … is exact判斷是否正合寫出 ∂M/∂y\partial M/\partial y 與 ∂N/∂x\partial N/\partial x
Find an integrating factor找積分因子F(x)F(x)、F(y)F(y) 或 xaybx^ay^b
Find a basis of solutions找基底給 y1,y2y_1, y_2(線性獨立)
Show that … are linearly independent證明線性獨立算 Wronskian ≠0\neq 0
by reduction of order用降階法y2=u y1y_2 = u\,y_1
by the method of undetermined coefficients用待定係數法照表猜 ypy_p
by variation of parameters用參數變異法套 WW 的公式
Classify the equation (order, linear, homogeneous)分類方程階數、線性與否、齊次與否
Sketch the direction field畫方向場用 isoclines f(x,y)=kf(x, y) = k
implicit / explicit solution隱解/顯解H(x,y)=cH(x, y) = c 也可以當答案
characteristic (auxiliary) equation特徵方程(輔助方程)Euler–Cauchy 叫 auxiliary
double root / complex conjugate roots重根/共軛複根
hence / therefore / thus因此寫在結論前
考前必看

英文答題句型:照抄就能寫完整

Answer Templates
白話講

不用寫漂亮的英文,每一步一句短句就夠了。老師要看的是你的步驟和判斷理由,句型照抄下面的就好。

什麼時候用句型
判斷型態The equation is separable / linear / exact / a Bernoulli equation with a=2a = 2.
寫標準式In standard form, y′+2xy=x2y' + \frac{2}{x}y = x^2, so p=2xp = \frac2x and r=x2r = x^2.
正合判別Since ∂M∂y=6xy=∂N∂x\frac{\partial M}{\partial y} = 6xy = \frac{\partial N}{\partial x}, the equation is exact.
不正合Since ∂M∂y≠∂N∂x\frac{\partial M}{\partial y} \neq \frac{\partial N}{\partial x}, the equation is not exact.
積分因子1N(∂M∂y−∂N∂x)=1x\frac1N\left(\frac{\partial M}{\partial y} - \frac{\partial N}{\partial x}\right) = \frac1x depends only on xx, so F=e∫dx/x=xF = e^{\int dx/x} = x.
變數變換Let u=y/xu = y/x. Then y=uxy = ux and y′=u+xu′y' = u + xu'.
兩邊積分Separating variables and integrating both sides, we obtain …
特徵方程The characteristic equation is λ2+2λ+5=0\lambda^2 + 2\lambda + 5 = 0, whose roots are λ=−1±2i\lambda = -1 \pm 2i.
齊次通解Hence the general solution of the homogeneous equation is yh=…y_h = \dots
修正規則Since e2xe^{2x} is a solution of the homogeneous equation, we try yp=Cxe2xy_p = Cxe^{2x} (modification rule).
比較係數Substituting ypy_p into the equation and comparing coefficients, we get C=4C = 4.
初始條件Applying the initial conditions y(0)=1, y′(0)=0y(0) = 1,\ y'(0) = 0, we find c1=1, c2=0c_1 = 1,\ c_2 = 0.
WronskianW(y1,y2)=y1y2′−y1′y2=2e−2x≠0W(y_1, y_2) = y_1y_2' - y_1'y_2 = 2e^{-2x} \neq 0, so y1,y2y_1, y_2 are linearly independent.
結論Therefore, the solution is y=…y = \dots

每一題結尾都寫一句 Therefore / Hence, …,把最後答案框起來。中間步驟寫數學式就好,不用每行都寫英文。

考前必看

最常扣分的 10 個地方

Common Mistakes
#錯在哪正確做法
1線性方程沒先除成標準式xy′+2y=x3xy' + 2y = x^3 → p=2x, r=x2p = \frac2x,\ r = x^2
2R-1、R-2、Bernoulli 算完沒換回 yy最後一行一定是 x,yx, y 的式子
3正合的答案只寫 uu,沒寫 =c= cu(x,y)=cu(x, y) = c
4積分因子 RR 與 R∗R^* 的分母對調F(x)F(x) 除以 NN;F(y)F(y) 除以 MM
5Bernoulli 換完 p,rp, r 忘了乘 (1−a)(1 - a)u′+(1−a) p u=(1−a) ru' + (1-a)\,p\,u = (1-a)\,r
6重根忘記乘 xx(EC 忘記乘 ln⁡x\ln x)常數個數要等於階數
7複數根寫成 cos⁡(3ix)\cos(3ix)ω\omega 是虛部的數字,不含 ii
8Euler–Cauchy 用 m2+am+bm^2 + am + bm2+(a−1)m+bm^2 + (a - 1)m + b
9待定係數撞到 yhy_h 沒修正先解 yhy_h 再猜;撞到就乘 xx 或 x2x^2
10初始條件只代進 yhy_h代進 y=yh+ypy = y_h + y_p
練習 01

一階線性 IVP

Practice: Linear First-Order
題目Solve the initial value problem x y′+2y=x3, y(1)=1x\,y' + 2y = x^3,\ y(1) = 1.先自己算,再看下面的詳解。
詳解
① 除以 xx 變標準式
y′+2x y=x2,p=2x,r=x2y' + \frac2x\,y = x^2,\qquad p = \frac2x,\quad r = x^2y′+2x y=x2,p=2x,r=x2\begin{aligned}&y' + \frac2x\,y = x^2, \\[2pt] &p = \frac2x, \\[2pt] &r = x^2\end{aligned}
② h=∫p dx=2ln⁡xh = \int p\,dx = 2\ln x,所以 eh=x2e^{h} = x^2
y=x−2[∫x2⋅x2 dx+c]=x−2[x55+c]=x35+cx2y = x^{-2}\left[\int x^2\cdot x^2\,dx + c\right] = x^{-2}\left[\frac{x^5}{5} + c\right] = \frac{x^3}{5} + \frac{c}{x^2}y=x−2[∫x2⋅x2 dx+c]=x−2[x55+c]=x35+cx2\begin{aligned}&y = x^{-2}\left[\int x^2\cdot x^2\,dx + c\right] \\[2pt] &\quad = x^{-2}\left[\frac{x^5}{5} + c\right] \\[2pt] &\quad = \frac{x^3}{5} + \frac{c}{x^2}\end{aligned}
③ 代 y(1)=1y(1) = 1
15+c=1  ⇒  c=45\frac15 + c = 1 \;\Rightarrow\; c = \frac45
結論y=x35+45x2y = \frac{x^3}{5} + \frac{4}{5x^2}
練習 02

正合方程

Practice: Exact Equation
題目Show that (ycos⁡x+2xey) dx+(sin⁡x+x2ey−1) dy=0(y\cos x + 2xe^y)\,dx + (\sin x + x^2e^y - 1)\,dy = 0 is exact and solve it.先自己算,再看下面的詳解。
詳解
① 判別
∂M∂y=cos⁡x+2xey=∂N∂x  ⇒  exact\frac{\partial M}{\partial y} = \cos x + 2xe^{y} = \frac{\partial N}{\partial x} \;\Rightarrow\; \text{exact}∂M∂y=cos⁡x+2xey=∂N∂x⇒  exact\begin{aligned}&\frac{\partial M}{\partial y} = \cos x + 2xe^{y} = \frac{\partial N}{\partial x} \\[2pt] &\Rightarrow\; \text{exact}\end{aligned}
② Step 1
u=∫(ycos⁡x+2xey) dx+k(y)=ysin⁡x+x2ey+k(y)u = \int (y\cos x + 2xe^{y})\,dx + k(y) = y\sin x + x^2e^{y} + k(y)u=∫(ycos⁡x+2xey) dx+k(y)=ysin⁡x+x2ey+k(y)\begin{aligned}&u = \int (y\cos x + 2xe^{y})\,dx + k(y) \\[2pt] &\quad = y\sin x + x^2e^{y} + k(y)\end{aligned}
③ Step 2
∂u∂y=sin⁡x+x2ey+k′(y)=sin⁡x+x2ey−1  ⇒  k(y)=−y\frac{\partial u}{\partial y} = \sin x + x^2e^{y} + k'(y) = \sin x + x^2e^{y} - 1 \;\Rightarrow\; k(y) = -y∂u∂y=sin⁡x+x2ey+k′(y)=sin⁡x+x2ey−1⇒  k(y)=−y\begin{aligned}&\frac{\partial u}{\partial y} = \sin x + x^2e^{y} + k'(y) \\[2pt] &\quad = \sin x + x^2e^{y} - 1 \\[2pt] &\Rightarrow\; k(y) = -y\end{aligned}
結論ysin⁡x+x2ey−y=cy\sin x + x^2e^y - y = c
練習 03

Bernoulli 方程

Practice: Bernoulli
題目Solve y′−y=−ex y2y' - y = -e^x\,y^2.先自己算,再看下面的詳解。
詳解
① a=2, p=−1, r=−exa = 2,\ p = -1,\ r = -e^x;令 u=y−1u = y^{-1}
u′+(1−2)(−1) u=(1−2)(−ex)  ⇒  u′+u=exu' + (1-2)(-1)\,u = (1-2)(-e^{x}) \;\Rightarrow\; u' + u = e^{x}u′+(1−2)(−1) u=(1−2)(−ex)⇒  u′+u=ex\begin{aligned}&u' + (1-2)(-1)\,u = (1-2)(-e^{x}) \\[2pt] &\Rightarrow\; u' + u = e^{x}\end{aligned}
② 線性公式,h=xh = x
u=e−x[∫exex dx+c]=ex2+c e−xu = e^{-x}\left[\int e^{x}e^{x}\,dx + c\right] = \frac{e^{x}}{2} + c\,e^{-x}u=e−x[∫exex dx+c]=ex2+c e−x\begin{aligned}&u = e^{-x}\left[\int e^{x}e^{x}\,dx + c\right] \\[2pt] &\quad = \frac{e^{x}}{2} + c\,e^{-x}\end{aligned}
③ 換回 y=1uy = \frac1u
y=112ex+c e−xy = \frac{1}{\frac12e^{x} + c\,e^{-x}}
結論y=112ex+c e−xy = \frac{1}{\frac12e^x + c\,e^{-x}}
練習 04

待定係數(共振)+初值

Practice: Undetermined Coefficients
題目Solve y′′+4y=8cos⁡2x, y(0)=1, y′(0)=0y'' + 4y = 8\cos 2x,\ y(0) = 1,\ y'(0) = 0.先自己算,再看下面的詳解。
詳解
① 齊次:λ=±2i\lambda = \pm2i
yh=c1cos⁡2x+c2sin⁡2xy_h = c_1\cos2x + c_2\sin2x
② cos⁡2x\cos 2x 在 yhy_h 裡(單根)→ 乘 xx
yp=x (Kcos⁡2x+Msin⁡2x)y_p = x\,(K\cos2x + M\sin2x)
③ 微分兩次代入,xx 的項抵銷
yp′′+4yp=−4Ksin⁡2x+4Mcos⁡2x=8cos⁡2x  ⇒  K=0, M=2y_p'' + 4y_p = -4K\sin2x + 4M\cos2x = 8\cos2x \;\Rightarrow\; K = 0,\ M = 2yp′′+4yp=−4Ksin⁡2x+4Mcos⁡2x=8cos⁡2x⇒  K=0, M=2\begin{aligned}&y_p'' + 4y_p = -4K\sin2x + 4M\cos2x \\[2pt] &\quad = 8\cos2x \\[2pt] &\Rightarrow\; K = 0,\ M = 2\end{aligned}
④ y=yh+2xsin⁡2xy = y_h + 2x\sin 2x;代 y(0)=1y(0) = 1 → c1=1c_1 = 1
⑤ y′=−2c1sin⁡2x+2c2cos⁡2x+2sin⁡2x+4xcos⁡2xy' = -2c_1\sin 2x + 2c_2\cos 2x + 2\sin 2x + 4x\cos 2x;y′(0)=2c2=0y'(0) = 2c_2 = 0 → c2=0c_2 = 0
結論y=cos⁡2x+2xsin⁡2xy = \cos 2x + 2x\sin 2x(振幅隨 xx 變大,這就是共振,圖在 m2-8)
練習 05

Euler–Cauchy(複數根)

Practice: Euler–Cauchy
題目Solve x2y′′+x y′+4y=0, y(1)=1, y′(1)=2x^2y'' + x\,y' + 4y = 0,\ y(1) = 1,\ y'(1) = 2.先自己算,再看下面的詳解。
詳解
① a=1, b=4a = 1,\ b = 4:輔助方程
m2+(1−1)m+4=m2+4=0  ⇒  m=±2i(μ=0, ν=2)m^2 + (1-1)m + 4 = m^2 + 4 = 0 \;\Rightarrow\; m = \pm 2i\quad(\mu = 0,\ \nu = 2)m2+(1−1)m+4=m2+4=0⇒  m=±2i(μ=0, ν=2)\begin{aligned}&m^2 + (1-1)m + 4 = m^2 + 4 = 0 \\[2pt] &\Rightarrow\; m = \pm 2i\quad(\mu = 0,\ \nu = 2)\end{aligned}
② 通解
y=c1cos⁡(2ln⁡x)+c2sin⁡(2ln⁡x)y = c_1\cos(2\ln x) + c_2\sin(2\ln x)
③ y(1)=c1=1y(1) = c_1 = 1(ln⁡1=0\ln 1 = 0)
④ y′=−2c1sin⁡(2ln⁡x)+2c2cos⁡(2ln⁡x)xy' = \frac{-2c_1\sin(2\ln x) + 2c_2\cos(2\ln x)}{x};y′(1)=2c2=2y'(1) = 2c_2 = 2 → c2=1c_2 = 1
結論y=cos⁡(2ln⁡x)+sin⁡(2ln⁡x)y = \cos(2\ln x) + \sin(2\ln x)
練習 06

參數變異

Practice: Variation of Parameters
題目Solve y′′+y=tan⁡xy'' + y = \tan x by variation of parameters.先自己算,再看下面的詳解。
詳解
① y1=cos⁡x, y2=sin⁡x, W=1y_1 = \cos x,\ y_2 = \sin x,\ W = 1
yp=−cos⁡x∫sin⁡xtan⁡x dx+sin⁡x∫cos⁡xtan⁡x dx\begin{aligned} y_p &= -\cos x\int\sin x\tan x\,dx \\ &\quad + \sin x\int\cos x\tan x\,dx \end{aligned}
② 第一個積分:sin⁡2xcos⁡x=sec⁡x−cos⁡x\frac{\sin^2 x}{\cos x} = \sec x - \cos x
∫sin⁡xtan⁡x dx=ln⁡∣sec⁡x+tan⁡x∣−sin⁡x\int\sin x\tan x\,dx = \ln|\sec x + \tan x| - \sin x
③ 第二個積分
∫cos⁡xtan⁡x dx=∫sin⁡x dx=−cos⁡x\int\cos x\tan x\,dx = \int\sin x\,dx = -\cos x
④ 代回,sin⁡xcos⁡x\sin x\cos x 兩項抵銷
yp=−cos⁡x ln⁡∣sec⁡x+tan⁡x∣y_p = -\cos x\,\ln|\sec x + \tan x|
結論y=c1cos⁡x+c2sin⁡x−cos⁡x ln⁡∣sec⁡x+tan⁡x∣y = c_1\cos x + c_2\sin x - \cos x\,\ln|\sec x + \tan x|
練習 07

三階非齊次

Practice: Third-Order
題目Find the general solution of y′′′−2y′′−y′+2y=4xy''' - 2y'' - y' + 2y = 4x.先自己算,再看下面的詳解。
詳解
① 分組因式分解
λ3−2λ2−λ+2=λ2(λ−2)−(λ−2)=(λ−2)(λ−1)(λ+1)\lambda^3 - 2\lambda^2 - \lambda + 2 = \lambda^2(\lambda - 2) - (\lambda - 2) = (\lambda - 2)(\lambda - 1)(\lambda + 1)λ3−2λ2−λ+2=λ2(λ−2)−(λ−2)=(λ−2)(λ−1)(λ+1)\begin{aligned}&\lambda^3 - 2\lambda^2 - \lambda + 2 \\[2pt] &\quad = \lambda^2(\lambda - 2) - (\lambda - 2) \\[2pt] &\quad = (\lambda - 2)(\lambda - 1)(\lambda + 1)\end{aligned}
② 齊次解
yh=c1e2x+c2ex+c3e−xy_h = c_1e^{2x} + c_2e^{x} + c_3e^{-x}
③ λ=0\lambda = 0 不是根 → 直接猜 yp=Ax+By_p = Ax + B;yp′=A, yp′′=yp′′′=0y_p' = A,\ y_p'' = y_p''' = 0
−A+2(Ax+B)=4x  ⇒  A=2, B=1-A + 2(Ax + B) = 4x \;\Rightarrow\; A = 2,\ B = 1−A+2(Ax+B)=4x⇒  A=2, B=1\begin{aligned}&-A + 2(Ax + B) = 4x \\[2pt] &\Rightarrow\; A = 2,\ B = 1\end{aligned}
結論y=c1e2x+c2ex+c3e−x+2x+1y = c_1e^{2x} + c_2e^x + c_3e^{-x} + 2x + 1
考前必看

進考場前最後五分鐘

Last Five Minutes
白話講

最後五分鐘不要再看新東西。只做三件事:

①看一次「30 秒判斷題型」,把七種一階、五種二階的認法在腦中跑一遍
②看一次「最常扣分的 10 個地方」
③確認帶了:列印的公式表、計算紙、筆

每題先寫型態判斷那一句(The equation is linear / exact / …)。就算後面算錯,判斷對的那一步也能拿到部分分數。

白話講堂・由 Atlas 產生。內容依據課程教材與官方教學大綱整理,不是老師的官方講義,請以課堂公告為準。