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Further Calculus

This chapter covers Advanced Higher Mathematics content.

When a function is defined implicitly (e.g., x2+y2=25x^2 + y^2 = 25), differentiate both sides with Respect to xxTreating yy as a function of xx.

ddx[yn]=nyn−1dydx\frac{d}{dx}[y^n] = ny^{n-1}\frac{dy}{dx}

This is the chain rule applied to y(x)ny(x)^n: ddx[yn]=nyn−1⋅y"(x)\frac{d}{dx}[y^n] = ny^{n-1} \cdot y"(x).

Example: Find dydx\dfrac{dy}{dx} for x2+y2=25x^2 + y^2 = 25.

2x+2ydydx=02x + 2y\frac{dy}{dx} = 0dydx=−xy\frac{dy}{dx} = -\frac{x}{y}

This makes geometric sense: on the upper semicircle (y>0y > 0), increasing xx decreases yyGiving A negative slope. On the lower semicircle (y<0y < 0), the slope is positive.

Example: Find dydx\dfrac{dy}{dx} for x3+y3=6xyx^3 + y^3 = 6xy.

Differentiate implicitly:

3x2+3y2dydx=6y+6xdydx3x^2 + 3y^2\frac{dy}{dx} = 6y + 6x\frac{dy}{dx}3y2dydx−6xdydx=6y−3x23y^2\frac{dy}{dx} - 6x\frac{dy}{dx} = 6y - 3x^2dydx(3y2−6x)=6y−3x2\frac{dy}{dx}(3y^2 - 6x) = 6y - 3x^2dydx=6y−3x23y2−6x=2y−x2y2−2x\frac{dy}{dx} = \frac{6y - 3x^2}{3y^2 - 6x} = \frac{2y - x^2}{y^2 - 2x}

Example: Find the tangent to x2+y2+2x−4y=11x^2 + y^2 + 2x - 4y = 11 at the point (1,2)(1, 2).

Verify: 1+4+2−8=−1≠111 + 4 + 2 - 8 = -1 \neq 11. The point is not on the curve. Let us find the gradient Function first:

2x+2ydydx+2−4dydx=02x + 2y\frac{dy}{dx} + 2 - 4\frac{dy}{dx} = 0(2y−4)dydx=−2x−2(2y - 4)\frac{dy}{dx} = -2x - 2dydx=−2x−22y−4=−x−1y−2\frac{dy}{dx} = \frac{-2x - 2}{2y - 4} = \frac{-x - 1}{y - 2}

Second derivatives implicitly. Differentiate dydx\frac{dy}{dx} again with respect to xxUsing The chain rule wherever yy appears.

If x=f(t)x = f(t) and y=g(t)y = g(t)Then:

dydx=dy/dtdx/dt=g′(t)f′(t)\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{g'(t)}{f'(t)}

This follows from the chain rule: dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}.

Second Derivative:

d2ydx2=ddx(dydx)=ddt(dydx)dx/dt\frac{d^2y}{dx^2} = \frac{d}{dx}\left(\frac{dy}{dx}\right) = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{dx/dt}

Example: A curve has parametric equations x=2cos⁡tx = 2\cos t, y=sin⁡2ty = \sin 2t. Find dydx\dfrac{dy}{dx} at t=π4t = \dfrac{\pi}{4}.

dxdt=−2sin⁡t,dydt=2cos⁡2t\frac{dx}{dt} = -2\sin t, \quad \frac{dy}{dt} = 2\cos 2tdydx=2cos⁡2t−2sin⁡t=−cos⁡2tsin⁡t\frac{dy}{dx} = \frac{2\cos 2t}{-2\sin t} = -\frac{\cos 2t}{\sin t}

At t=π4t = \dfrac{\pi}{4}:

dydx=−cos⁡(π/2)sin⁡(π/4)=−01/2=0\frac{dy}{dx} = -\frac{\cos(\pi/2)}{\sin(\pi/4)} = -\frac{0}{1/\sqrt{2}} = 0

Example: Find d2ydx2\frac{d^2y}{dx^2} for x=t2x = t^2, y=t3y = t^3.

dydx=3t22t=3t2\frac{dy}{dx} = \frac{3t^2}{2t} = \frac{3t}{2}d2ydx2=d/dt(3t/2)dx/dt=3/22t=34t\frac{d^2y}{dx^2} = \frac{d/dt(3t/2)}{dx/dt} = \frac{3/2}{2t} = \frac{3}{4t}

Differentiation of Inverse Trigonometric Functions

Section titled “Differentiation of Inverse Trigonometric Functions”
ddx[arcsin⁡x]=11−x2,∣x∣<1\frac{d}{dx}[\arcsin x] = \frac{1}{\sqrt{1 - x^2}}, \quad |x| < 1ddx[arccos⁡x]=−11−x2,∣x∣<1\frac{d}{dx}[\arccos x] = \frac{-1}{\sqrt{1 - x^2}}, \quad |x| < 1ddx[arctan⁡x]=11+x2\frac{d}{dx}[\arctan x] = \frac{1}{1 + x^2}

Proof that ddx[arctan⁡x]=11+x2\frac{d}{dx}[\arctan x] = \frac{1}{1+x^2}. Let y=arctan⁡xy = \arctan xSo x=tan⁡yx = \tan y. Differentiating implicitly: 1=sec⁡2y⋅dydx1 = \sec^2 y \cdot \frac{dy}{dx}Giving dydx=1sec⁡2y=11+tan⁡2y=11+x2\frac{dy}{dx} = \frac{1}{\sec^2 y} = \frac{1}{1 + \tan^2 y} = \frac{1}{1 + x^2}.

Example: Differentiate f(x)=arcsin⁡(3x)f(x) = \arcsin(3x).

F′(x)=11−(3x)2⋅3=31−9x2F'(x) = \frac{1}{\sqrt{1 - (3x)^2}} \cdot 3 = \frac{3}{\sqrt{1 - 9x^2}}

For functions of the form y=[f(x)]g(x)y = [f(x)]^{g(x)}Take natural logarithms first:

ln⁡y=g(x)ln⁡f(x)\ln y = g(x) \ln f(x)

Then differentiate implicitly.

Example: Differentiate y=xxy = x^x.

ln⁡y=xln⁡x\ln y = x \ln x1ydydx=ln⁡x+x⋅1x=ln⁡x+1\frac{1}{y}\frac{dy}{dx} = \ln x + x \cdot \frac{1}{x} = \ln x + 1dydx=y(ln⁡x+1)=xx(ln⁡x+1)\frac{dy}{dx} = y(\ln x + 1) = x^x(\ln x + 1)

Example: Differentiate y=xsin⁡xy = x^{\sin x}.

ln⁡y=sin⁡x⋅ln⁡x\ln y = \sin x \cdot \ln x1ydydx=cos⁡x⋅ln⁡x+sin⁡x⋅1x\frac{1}{y}\frac{dy}{dx} = \cos x \cdot \ln x + \sin x \cdot \frac{1}{x}dydx=xsin⁡x ⁣(cos⁡xln⁡x+sin⁡xx)\frac{dy}{dx} = x^{\sin x}\!\left(\cos x \ln x + \frac{\sin x}{x}\right)

Related rates problems involve finding the rate of change of one quantity given the rate of change Of a related quantity.

Example: A ladder 5 m long leans against a wall. The bottom slides away at 0.5 m/s. How fast is The top sliding down when the bottom is 3 m from the wall?

Let xx be the distance from the wall and yy be the height. Then x2+y2=25x^2 + y^2 = 25.

Differentiate: 2xdxdt+2ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0.

When x=3x = 3: y=25−9=4y = \sqrt{25 - 9} = 4.

2(3)(0.5) + 2(4)\frac{dy}{dt} = 0 \implies 3 + 8\frac{dy}{dt} = 0 \implies \frac{dy}{dt} = -\frac{3}{8} \mathrm{ m/s
∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du

Proof. By the product rule: ddx[uv]=u′v+uv′\frac{d}{dx}[uv] = u'v + uv'So uv′=ddx[uv]−u′vuv' = \frac{d}{dx}[uv] - u'v. Integrating both sides: ∫uv′ dx=uv−∫u′v dx\int uv'\,dx = uv - \int u'v\,dx.

LIATE rule for choosing uu (in order of priority): Logarithmic, Inverse trig, Algebraic, Trigonometric, Exponential. Choose uu as the function that appears earliest in this list.

Example: Evaluate ∫xe2x dx\int x e^{2x} \, dx.

Let u = x$$dv = e^{2x} dx. Then du = dx$$v = \dfrac{e^{2x}}{2}.

∫xe2x dx=x⋅e2x2−∫e2x2 dx=xe2x2−e2x4+C=e2x(2x−1)4+C\int x e^{2x} \, dx = x \cdot \frac{e^{2x}}{2} - \int \frac{e^{2x}}{2} \, dx = \frac{x e^{2x}}{2} - \frac{e^{2x}}{4} + C = \frac{e^{2x}(2x - 1)}{4} + C

Example: Evaluate ∫x2cos⁡x dx\int x^2 \cos x \, dx.

Let u = x^2$$dv = \cos x \, dx. Then du = 2x \, dx$$v = \sin x.

=x2sin⁡x−∫2xsin⁡x dx= x^2 \sin x - \int 2x \sin x \, dx

Apply integration by parts again for ∫xsin⁡x dx\int x \sin x \, dx:

Let u = x$$dv = \sin x \, dx. Then du = dx$$v = -\cos x.

∫xsin⁡x dx=−xcos⁡x+∫cos⁡x dx=−xcos⁡x+sin⁡x\int x \sin x \, dx = -x\cos x + \int \cos x \, dx = -x\cos x + \sin x

So:

∫x2cos⁡x dx=x2sin⁡x−2(−xcos⁡x+sin⁡x)+C=x2sin⁡x+2xcos⁡x−2sin⁡x+C\int x^2 \cos x \, dx = x^2 \sin x - 2(-x\cos x + \sin x) + C = x^2 \sin x + 2x\cos x - 2\sin x + C

Some integrals require integration by parts twice, then solving algebraically.

Example: Evaluate ∫excos⁡x dx\int e^x \cos x \, dx.

Let u = e^x$$dv = \cos x\,dx. Then du = e^x\,dx$$v = \sin x.

I=exsin⁡x−∫exsin⁡x dxI = e^x \sin x - \int e^x \sin x\,dx

Apply parts again for ∫exsin⁡x dx\int e^x \sin x\,dx: u = e^x$$dv = \sin x\,dx.

∫exsin⁡x dx=−excos⁡x+∫excos⁡x dx=−excos⁡x+I\int e^x \sin x\,dx = -e^x \cos x + \int e^x \cos x\,dx = -e^x \cos x + I

Substituting back:

I=exsin⁡x−(−excos⁡x+I)=exsin⁡x+excos⁡x−II = e^x \sin x - (-e^x \cos x + I) = e^x \sin x + e^x \cos x - I2I=ex(sin⁡x+cos⁡x)2I = e^x(\sin x + \cos x)I=ex(sin⁡x+cos⁡x)2+CI = \frac{e^x(\sin x + \cos x)}{2} + C\int f(g(x))g'(x) \, dx = \int f(u) \, du \quad \mathrm{where u = g(x)

Example: Evaluate ∫xx2+1 dx\int \dfrac{x}{x^2 + 1} \, dx.

Let u=x2+1u = x^2 + 1So du=2x dxdu = 2x \, dxGiving 12du=x dx\dfrac{1}{2} du = x \, dx.

∫xx2+1 dx=12∫duu=12ln⁡∣u∣+C=12ln⁡(x2+1)+C\int \frac{x}{x^2 + 1} \, dx = \frac{1}{2}\int \frac{du}{u} = \frac{1}{2}\ln|u| + C = \frac{1}{2}\ln(x^2 + 1) + C

When using substitution in a definite integral, you must change the limits.

Example: Evaluate ∫012xx2+1 dx\displaystyle\int_0^1 \frac{2x}{x^2 + 1}\,dx.

Let u=x2+1u = x^2 + 1. When x = 0$$u = 1. When x = 1$$u = 2.

∫012xx2+1 dx=∫12duu=[ln⁡u]12=ln⁡2−ln⁡1=ln⁡2\int_0^1 \frac{2x}{x^2 + 1}\,dx = \int_1^2 \frac{du}{u} = [\ln u]_1^2 = \ln 2 - \ln 1 = \ln 2

Rational functions can be decomposed using partial fractions to make them easier to integrate.

Example: Evaluate ∫2x+1(x+1)(x−2) dx\displaystyle\int \frac{2x + 1}{(x + 1)(x - 2)} \, dx.

2x+1(x+1)(x−2)=Ax+1+Bx−2\frac{2x + 1}{(x + 1)(x - 2)} = \frac{A}{x + 1} + \frac{B}{x - 2}2x+1=A(x−2)+B(x+1)2x + 1 = A(x - 2) + B(x + 1)

x=−1x = -1: −2+1=A(−3)-2 + 1 = A(-3)So A=13A = \dfrac{1}{3}.

x=2x = 2: 4+1=B(3)4 + 1 = B(3)So B=53B = \dfrac{5}{3}.

∫2x+1(x+1)(x−2) dx=13∫dxx+1+53∫dxx−2=13ln⁡∣x+1∣+53ln⁡∣x−2∣+C\int \frac{2x + 1}{(x + 1)(x - 2)} \, dx = \frac{1}{3}\int \frac{dx}{x + 1} + \frac{5}{3}\int \frac{dx}{x - 2} = \frac{1}{3}\ln|x + 1| + \frac{5}{3}\ln|x - 2| + C∫tan⁡x dx=−ln⁡∣cos⁡x∣+C=ln⁡∣sec⁡x∣+C\int \tan x \, dx = -\ln|\cos x| + C = \ln|\sec x| + C∫cot⁡x dx=ln⁡∣sin⁡x∣+C\int \cot x \, dx = \ln|\sin x| + C∫sec⁡x dx=ln⁡∣sec⁡x+tan⁡x∣+C\int \sec x \, dx = \ln|\sec x + \tan x| + C

Example: Evaluate ∫tan⁡2x dx\int \tan^2 x \, dx.

∫tan⁡2x dx=∫(sec⁡2x−1) dx=tan⁡x−x+C\int \tan^2 x \, dx = \int (\sec^2 x - 1) \, dx = \tan x - x + C

Example: Evaluate ∫dxsin⁡2x+4cos⁡2x\displaystyle\int \frac{dx}{\sin^2 x + 4\cos^2 x}.

Divide numerator and denominator by cos⁡2x\cos^2 x:

=∫sec⁡2xtan⁡2x+4 dx= \int \frac{\sec^2 x}{\tan^2 x + 4} \, dx

Let u = \tan x$$du = \sec^2 x \, dx:

=∫duu2+4=12arctan⁡(u2)+C=12arctan⁡(tan⁡x2)+C= \int \frac{du}{u^2 + 4} = \frac{1}{2}\arctan\left(\frac{u}{2}\right) + C = \frac{1}{2}\arctan\left(\frac{\tan x}{2}\right) + C

The volume generated by rotating y=f(x)y = f(x) about the xx-axis from x=ax = a to x=bx = b:

V=π∫ab[f(x)]2 dxV = \pi \int_a^b [f(x)]^2 \, dx

The volume generated by rotating about the yy-axis:

V=π∫cd[f−1(y)]2 dyV = \pi \int_c^d [f^{-1}(y)]^2 \, dy

Example: Find the volume generated by rotating y=xy = \sqrt{x} about the xx-axis from x=0x = 0 to x=4x = 4.

V=π∫04x dx=π[x22]04=8πV = \pi \int_0^4 x \, dx = \pi\left[\frac{x^2}{2}\right]_0^4 = 8\pi

Separable Equations: Equations of the form dydx=f(x)g(y)\dfrac{dy}{dx} = f(x)g(y) can be solved by Separating variables:

∫dyg(y)=∫f(x) dx\int \frac{dy}{g(y)} = \int f(x) \, dx

Example: Solve dydx=xy\dfrac{dy}{dx} = \dfrac{x}{y} with y(0)=2y(0) = 2.

Y dy=x dxY \, dy = x \, dx∫y dy=∫x dx\int y \, dy = \int x \, dxy22=x22+C\frac{y^2}{2} = \frac{x^2}{2} + CY2=x2+2CY^2 = x^2 + 2C

Using y(0)=2y(0) = 2: 4=0+2C4 = 0 + 2CSo C=2C = 2.

Y2=x2+4Y^2 = x^2 + 4

Since y(0)=2>0y(0) = 2 > 0: y=x2+4y = \sqrt{x^2 + 4}.

Equations of the form:

dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x)

Integrating Factor: μ(x)=e∫P(x) dx\mu(x) = e^{\int P(x) \, dx}

Multiply through by the integrating factor:

ddx[μy]=μQ\frac{d}{dx}[\mu y] = \mu QY=1μ∫μQ dxY = \frac{1}{\mu}\int \mu Q \, dx

Why this works. We want to write the left side as the derivative of a product. If we multiply by μ\mu:

μdydx+μPy=μQ\mu\frac{dy}{dx} + \mu P y = \mu Q

This is ddx[μy]\frac{d}{dx}[\mu y] provided μ′=μP\mu' = \mu PI.e., μ=e∫P dx\mu = e^{\int P\,dx}.

Example: Solve dydx+3y=6e−3x\dfrac{dy}{dx} + 3y = 6e^{-3x}.

Integrating factor: μ=e∫3 dx=e3x\mu = e^{\int 3 \, dx} = e^{3x}.

E3xdydx+3e3xy=6E^{3x}\frac{dy}{dx} + 3e^{3x}y = 6ddx[e3xy]=6\frac{d}{dx}[e^{3x}y] = 6E3xy=6x+CE^{3x}y = 6x + CY=e−3x(6x+C)Y = e^{-3x}(6x + C)

Homogeneous equations with constant coefficients:

Ad2ydx2+bdydx+cy=0A\frac{d^2y}{dx^2} + b\frac{dy}{dx} + cy = 0

Try y=emxy = e^{mx}: the auxiliary equation is am2+bm+c=0am^2 + bm + c = 0.

Case 1: Two distinct real roots m1,m2m_1, m_2:

Y=Aem1x+Bem2xY = Ae^{m_1 x} + Be^{m_2 x}

Case 2: Repeated root mm:

Y=(Ax+B)emxY = (Ax + B)e^{mx}

Case 3: Complex roots m=α±βim = \alpha \pm \beta i:

Y=eαx(Acos⁡βx+Bsin⁡βx)Y = e^{\alpha x}(A\cos\beta x + B\sin\beta x)

Why the complex case produces sines and cosines. If m=α+βim = \alpha + \beta iThen e(α+βi)x=eαx(cos⁡βx+isin⁡βx)e^{(\alpha+\beta i)x} = e^{\alpha x}(\cos\beta x + i\sin\beta x). Since the original DE has real Coefficients, both e(α+βi)xe^{(\alpha+\beta i)x} and e(α−βi)xe^{(\alpha-\beta i)x} are solutions. Their linear Combinations give eαxcos⁡βxe^{\alpha x}\cos\beta x and eαxsin⁡βxe^{\alpha x}\sin\beta x.

Example: Solve d2ydx2−5dydx+6y=0\dfrac{d^2y}{dx^2} - 5\dfrac{dy}{dx} + 6y = 0.

Auxiliary equation: m2−5m+6=0m^2 - 5m + 6 = 0So (m−2)(m−3)=0(m - 2)(m - 3) = 0Giving m=2,3m = 2, 3.

Y=Ae2x+Be3xY = Ae^{2x} + Be^{3x}

Example: Solve d2ydx2+4y=0\dfrac{d^2y}{dx^2} + 4y = 0.

Auxiliary equation: m2+4=0m^2 + 4 = 0So m=±2im = \pm 2i.

Y=Acos⁡2x+Bsin⁡2xY = A\cos 2x + B\sin 2x

Example: Solve d2ydx2+6dydx+9y=0\dfrac{d^2y}{dx^2} + 6\dfrac{dy}{dx} + 9y = 0.

Auxiliary equation: m2+6m+9=0m^2 + 6m + 9 = 0So (m+3)2=0(m + 3)^2 = 0Giving m=−3m = -3 (repeated).

Y=(Ax+B)e−3xY = (Ax + B)e^{-3x}Ad2ydx2+bdydx+cy=f(x)A\frac{d^2y}{dx^2} + b\frac{dy}{dx} + cy = f(x)

General Solution: y=yh+ypy = y_h + y_p (complementary function + particular integral).

Method for finding ypy_p: Guess the form of ypy_p based on f(x)f(x).

f(x)f(x)Guess for ypy_p
ekxe^{kx}CekxCe^{kx} (if kk is not a root)
kx+bkx + bAx+BAx + B
cos⁡kx\cos kx or sin⁡kx\sin kxAcos⁡kx+Bsin⁡kxA\cos kx + B\sin kx

Example: Solve d2ydx2−3dydx+2y=4e3x\dfrac{d^2y}{dx^2} - 3\dfrac{dy}{dx} + 2y = 4e^{3x}.

Complementary function: m2−3m+2=0m^2 - 3m + 2 = 0So m=1,2m = 1, 2.

Yh=Aex+Be2xY_h = Ae^x + Be^{2x}

For the particular integral, try yp=Ce3xy_p = Ce^{3x}:

9Ce3x−9Ce3x+2Ce3x=4e3x9Ce^{3x} - 9Ce^{3x} + 2Ce^{3x} = 4e^{3x}2C=4  ⟹  C=22C = 4 \implies C = 2Yp=2e3xY_p = 2e^{3x}

General solution: y=Aex+Be2x+2e3xy = Ae^x + Be^{2x} + 2e^{3x}.


The Maclaurin series expands a function as a power series about x=0x = 0:

F(x)=f(0)+f′(0)x+f′′(0)2!x2+f′′′(0)3!x3+⋯=∑n=0∞f(n)(0)n!xnF(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 + \cdots = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!}x^nEx=1+x+x22!+x33!+⋯E^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdotssin⁡x=x−x33!+x55!−⋯\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \cdotscos⁡x=1−x22!+x44!−⋯\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \cdotsln⁡(1+x)=x−x22+x33−x44+⋯ ,∣x∣≤1,x≠−1\ln(1 + x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \cdots, \quad |x| \leq 1, x \neq -1(1+x)n=1+nx+n(n−1)2!x2+n(n−1)(n−2)3!x3+⋯ ,∣x∣<1(1 + x)^n = 1 + nx + \frac{n(n-1)}{2!}x^2 + \frac{n(n-1)(n-2)}{3!}x^3 + \cdots, \quad |x| < 1

Example: Find the Maclaurin series for f(x)=e−x2f(x) = e^{-x^2} up to the term in x6x^6.

Substitute −x2-x^2 into the series for eue^u:

E−x2=1+(−x2)+(−x2)22!+(−x2)33!+⋯E^{-x^2} = 1 + (-x^2) + \frac{(-x^2)^2}{2!} + \frac{(-x^2)^3}{3!} + \cdots=1−x2+x42−x66+⋯= 1 - x^2 + \frac{x^4}{2} - \frac{x^6}{6} + \cdots

Limits: Maclaurin series can be used to evaluate limits that are indeterminate.

Example: Evaluate lim⁡x→0ex−1−xx2\displaystyle\lim_{x \to 0} \frac{e^x - 1 - x}{x^2}.

Ex−1−x=(1+x+x22+⋯ )−1−x=x22+⋯E^x - 1 - x = \left(1 + x + \frac{x^2}{2} + \cdots\right) - 1 - x = \frac{x^2}{2} + \cdotsex−1−xx2=x22+⋯x2=12+⋯→12\frac{e^x - 1 - x}{x^2} = \frac{\frac{x^2}{2} + \cdots}{x^2} = \frac{1}{2} + \cdots \to \frac{1}{2}

Integration of Series:

Example: Find ∫00.5e−x2 dx\displaystyle\int_0^{0.5} e^{-x^2} \, dx to 4 decimal places.

E−x2≈1−x2+x42−x66E^{-x^2} \approx 1 - x^2 + \frac{x^4}{2} - \frac{x^6}{6}∫00.5e−x2 dx≈[x−x33+x510−x742]00.5\int_0^{0.5} e^{-x^2} \, dx \approx \left[x - \frac{x^3}{3} + \frac{x^5}{10} - \frac{x^7}{42}\right]_0^{0.5}=0.5−0.1253+0.0312510−0.007812542= 0.5 - \frac{0.125}{3} + \frac{0.03125}{10} - \frac{0.0078125}{42}=0.5−0.04167+0.003125−0.000186=0.46127= 0.5 - 0.04167 + 0.003125 - 0.000186 = 0.46127

See the examples integrated throughout the sections above.

  1. Forgetting the chain rule in implicit differentiation: When differentiating y3y^3The result is 3y2dydx3y^2 \dfrac{dy}{dx}Not 3y23y^2.

  2. Wrong choice of uu in integration by parts: Follow the LIATE rule. Choosing algebraic functions as dvdv instead of uu leads to more complicated integrals.

  3. Missing the constant of integration: Always include +C+C for indefinite integrals.

  4. Incorrect auxiliary equation: For d2ydx2+4y=0\dfrac{d^2y}{dx^2} + 4y = 0The auxiliary equation is m2+4=0m^2 + 4 = 0Not m2+4m=0m^2 + 4m = 0.

  5. Domain restrictions in Maclaurin series: The series for ln⁡(1+x)\ln(1 + x) is valid for −1<x≤1-1 < x \le 1Not all xx.

  6. Forgetting to change limits in definite substitution: When u=g(x)u = g(x)The new limits are u(a)u(a) and u(b)u(b)Not aa and bb.

  7. Not checking that the particular integral guess works: If your guess for ypy_p contains a term already in yhy_hMultiply by xx and try again.


  1. Find dydx\dfrac{dy}{dx} for x3+xy2+y3=7x^3 + xy^2 + y^3 = 7.

  2. Evaluate ∫x2e−x dx\displaystyle\int x^2 e^{-x} \, dx by parts.

  3. Solve the differential equation dydx=2x+13y−2\dfrac{dy}{dx} = \dfrac{2x + 1}{3y - 2} with y(0)=1y(0) = 1.

  4. Find the Maclaurin series for f(x)=cos⁡(2x)f(x) = \cos(2x) up to the term in x6x^6.

  5. Solve d2ydx2+2dydx+y=0\dfrac{d^2y}{dx^2} + 2\dfrac{dy}{dx} + y = 0.

  6. A curve has parametric equations x = t^2$$y = t^3 - 3t. Find the coordinates of the stationary points.

  7. Evaluate ∫01dx1+x3\displaystyle\int_0^1 \frac{dx}{1 + x^3} by first finding the partial fraction decomposition.

  8. Solve dydx+2yx=x3\dfrac{dy}{dx} + \dfrac{2y}{x} = x^3 using an integrating factor.

  9. Solve d2ydx2−4y=2e3x\dfrac{d^2y}{dx^2} - 4y = 2e^{3x}.

  10. Find the volume of revolution when y=sin⁡xy = \sin x is rotated about the xx-axis from x=0x = 0 to x=πx = \pi.

  11. Evaluate ∫exsin⁡x dx\displaystyle\int e^x \sin x \, dx using cyclic integration by parts.

  12. Use Maclaurin series to evaluate lim⁡x→01−cos⁡xx2\displaystyle\lim_{x \to 0} \frac{1 - \cos x}{x^2}.

This topic covers the mathematical techniques and concepts related to further calculus, including key theorems, methods, and problem-solving approaches.

Key concepts include:

  • differentiation from first principles
  • product, quotient, and chain rules
  • integration techniques (by parts, substitution)
  • differential equations
  • applications to kinematics

Regular practice with a variety of question types is essential to build fluency and confidence in applying these mathematical techniques.