Parametric Equations x(t)x(t)x(t), y(t)y(t)y(t)Curve defined by: x = f(t), y = g(t), t ∈ [a, b]Parametric Equations $x(t)$, $y(t)$
dydx=dydtdxdt\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}dxdy=dtdxdtdydydx=dy/dtdx/dt=g′(t)f′(t)\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{g'(t)}{f'(t)}dxdy=dx/dtdy/dt=f′(t)g′(t)$\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}$
d2ydx2=ddt(dydx)dxdt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(\frac{dy}{dx})}{\frac{dx}{dt}}dx2d2y=dtdxdtd(dxdy)d2ydx2=ddt(dydx)dx/dt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{dx/dt}dx2d2y=dx/dtdtd(dxdy)$\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(\frac{dy}{dx})}{\frac{dx}{dt}}$
Arc Length = ∫ab(dxdt)2+(dydt)2dt\int_{a}^{b} \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2} dt∫ab(dtdx)2+(dtdy)2dtL=∫ab(f′(t))2+(g′(t))2 dtL = \int_a^b \sqrt{(f'(t))^2 + (g'(t))^2}\,dtL=∫ab(f′(t))2+(g′(t))2dtArc Length = $\int_{a}^{b} \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2} dt$
Vector-valued Function r(t)=⟨x(t),y(t)⟩\mathbf{r}(t) = \langle x(t), y(t) \rangler(t)=⟨x(t),y(t)⟩r⃗(t)=⟨x(t),y(t)⟩\vec{r}(t) = \langle x(t), y(t) \rangler(t)=⟨x(t),y(t)⟩Vector-Valued Function $\mathbf{r}(t) = \langle x(t), y(t) \rangle$
Integral Of r(t)=⟨∫x(t)dt,∫y(t)dt⟩\mathbf{r}(t) = \langle \int x(t)dt, \int y(t)dt \rangler(t)=⟨∫x(t)dt,∫y(t)dt⟩∫r⃗(t)dt=⟨∫x(t)dt,∫y(t)dt⟩\int \vec{r}(t)dt = \langle \int x(t)dt, \int y(t)dt \rangle∫r(t)dt=⟨∫x(t)dt,∫y(t)dt⟩Integral of $\mathbf{r}(t) = \langle \int x(t)dt, \int y(t)dt \rangle$
Position, Velocity, Acceleration Vectors v⃗(t)=r⃗′(t)\vec{v}(t) = \vec{r}'(t)v(t)=r′(t) a⃗(t)=r⃗′′(t)\vec{a}(t) = \vec{r}''(t)a(t)=r′′(t) Speed = ∣v⃗(t)∣|\vec{v}(t)|∣v(t)∣ Position, Velocity, Acceleration Vectors
Polar Coordinates (r,θ)(r, \theta)(r,θ)x=rcosθ,y=rsinθx = r\cos\theta, \quad y = r\sin\thetax=rcosθ,y=rsinθPolar Coordinates $(r, \theta)$
Dy/dx In Polar Formdydx=r′sinθ+rcosθr′cosθ−rsinθ\frac{dy}{dx} = \frac{r'\sin\theta + r\cos\theta}{r'\cos\theta - r\sin\theta}dxdy=r′cosθ−rsinθr′sinθ+rcosθ where r′=drdθr' = \frac{dr}{d\theta}r′=dθdrdy/dx in Polar Form
Area = 12∫αβ[r(θ)]2dθ\frac{1}{2} \int_{\alpha}^{\beta} [r(\theta)]^2 d\theta21∫αβ[r(θ)]2dθA=12∫αβ[r(θ)]2dθA = \frac{1}{2}\int_\alpha^\beta [r(\theta)]^2 d\thetaA=21∫αβ[r(θ)]2dθArea = $\frac{1}{2} \int_{\alpha}^{\beta} [r(\theta)]^2 d\theta$
Area = 12∫αβ([R(θ)]2−[r(θ)]2)dθ\frac{1}{2} \int_{\alpha}^{\beta} ([R(\theta)]^2 - [r(\theta)]^2) d\theta21∫αβ([R(θ)]2−[r(θ)]2)dθA=12∫αβ([R(θ)]2−[r(θ)]2)dθA = \frac{1}{2}\int_\alpha^\beta ([R(\theta)]^2 - [r(\theta)]^2)d\thetaA=21∫αβ([R(θ)]2−[r(θ)]2)dθ where R(θ) ≥ r(θ) on [alpha, β].Area = $\frac{1}{2} \int_{\alpha}^{\beta} ([R(\theta)]^2 - [r(\theta)]^2) d\theta$
Arc Length = ∫αβ[r(θ)]2+(drdθ)2dθ\int_{\alpha}^{\beta} \sqrt{[r(\theta)]^2 + (\frac{dr}{d\theta})^2} d\theta∫αβ[r(θ)]2+(dθdr)2dθL=∫αβr2+(drdθ)2 dθL = \int_\alpha^\beta \sqrt{r^2 + \left(\frac{dr}{d\theta}\right)^2}\,d\thetaL=∫αβr2+(dθdr)2dθArc Length = $\int_{\alpha}^{\beta} \sqrt{[r(\theta)]^2 + (\frac{dr}{d\theta})^2} d\theta$
Parametric Equations x(t)x(t)x(t), y(t)y(t)y(t)Curve defined by: x = f(t), y = g(t), t ∈ [a, b]Parametric Equations $x(t)$, $y(t)$
dydx=dydtdxdt\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}dxdy=dtdxdtdydydx=dy/dtdx/dt=g′(t)f′(t)\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{g'(t)}{f'(t)}dxdy=dx/dtdy/dt=f′(t)g′(t)$\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}$
d2ydx2=ddt(dydx)dxdt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(\frac{dy}{dx})}{\frac{dx}{dt}}dx2d2y=dtdxdtd(dxdy)d2ydx2=ddt(dydx)dx/dt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{dx/dt}dx2d2y=dx/dtdtd(dxdy)$\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(\frac{dy}{dx})}{\frac{dx}{dt}}$
Arc Length = ∫ab(dxdt)2+(dydt)2dt\int_{a}^{b} \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2} dt∫ab(dtdx)2+(dtdy)2dtL=∫ab(f′(t))2+(g′(t))2 dtL = \int_a^b \sqrt{(f'(t))^2 + (g'(t))^2}\,dtL=∫ab(f′(t))2+(g′(t))2dtArc Length = $\int_{a}^{b} \sqrt{(\frac{dx}{dt})^2 + (\frac{dy}{dt})^2} dt$
Vector-valued Function r(t)=⟨x(t),y(t)⟩\mathbf{r}(t) = \langle x(t), y(t) \rangler(t)=⟨x(t),y(t)⟩r⃗(t)=⟨x(t),y(t)⟩\vec{r}(t) = \langle x(t), y(t) \rangler(t)=⟨x(t),y(t)⟩Vector-Valued Function $\mathbf{r}(t) = \langle x(t), y(t) \rangle$
Integral Of r(t)=⟨∫x(t)dt,∫y(t)dt⟩\mathbf{r}(t) = \langle \int x(t)dt, \int y(t)dt \rangler(t)=⟨∫x(t)dt,∫y(t)dt⟩∫r⃗(t)dt=⟨∫x(t)dt,∫y(t)dt⟩\int \vec{r}(t)dt = \langle \int x(t)dt, \int y(t)dt \rangle∫r(t)dt=⟨∫x(t)dt,∫y(t)dt⟩Integral of $\mathbf{r}(t) = \langle \int x(t)dt, \int y(t)dt \rangle$
Position, Velocity, Acceleration Vectors v⃗(t)=r⃗′(t)\vec{v}(t) = \vec{r}'(t)v(t)=r′(t) a⃗(t)=r⃗′′(t)\vec{a}(t) = \vec{r}''(t)a(t)=r′′(t) Speed = ∣v⃗(t)∣|\vec{v}(t)|∣v(t)∣ Position, Velocity, Acceleration Vectors
Polar Coordinates (r,θ)(r, \theta)(r,θ)x=rcosθ,y=rsinθx = r\cos\theta, \quad y = r\sin\thetax=rcosθ,y=rsinθPolar Coordinates $(r, \theta)$
Dy/dx In Polar Formdydx=r′sinθ+rcosθr′cosθ−rsinθ\frac{dy}{dx} = \frac{r'\sin\theta + r\cos\theta}{r'\cos\theta - r\sin\theta}dxdy=r′cosθ−rsinθr′sinθ+rcosθ where r′=drdθr' = \frac{dr}{d\theta}r′=dθdrdy/dx in Polar Form
Area = 12∫αβ[r(θ)]2dθ\frac{1}{2} \int_{\alpha}^{\beta} [r(\theta)]^2 d\theta21∫αβ[r(θ)]2dθA=12∫αβ[r(θ)]2dθA = \frac{1}{2}\int_\alpha^\beta [r(\theta)]^2 d\thetaA=21∫αβ[r(θ)]2dθArea = $\frac{1}{2} \int_{\alpha}^{\beta} [r(\theta)]^2 d\theta$
Area = 12∫αβ([R(θ)]2−[r(θ)]2)dθ\frac{1}{2} \int_{\alpha}^{\beta} ([R(\theta)]^2 - [r(\theta)]^2) d\theta21∫αβ([R(θ)]2−[r(θ)]2)dθA=12∫αβ([R(θ)]2−[r(θ)]2)dθA = \frac{1}{2}\int_\alpha^\beta ([R(\theta)]^2 - [r(\theta)]^2)d\thetaA=21∫αβ([R(θ)]2−[r(θ)]2)dθ where R(θ) ≥ r(θ) on [alpha, β].Area = $\frac{1}{2} \int_{\alpha}^{\beta} ([R(\theta)]^2 - [r(\theta)]^2) d\theta$
Arc Length = ∫αβ[r(θ)]2+(drdθ)2dθ\int_{\alpha}^{\beta} \sqrt{[r(\theta)]^2 + (\frac{dr}{d\theta})^2} d\theta∫αβ[r(θ)]2+(dθdr)2dθL=∫αβr2+(drdθ)2 dθL = \int_\alpha^\beta \sqrt{r^2 + \left(\frac{dr}{d\theta}\right)^2}\,d\thetaL=∫αβr2+(dθdr)2dθArc Length = $\int_{\alpha}^{\beta} \sqrt{[r(\theta)]^2 + (\frac{dr}{d\theta})^2} d\theta$