Sem 2 Stewart Flashcards

1
Q

method for 1st order differential equation

A

separating the variables

integrating factor if variables cannot be seperated

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2
Q

method for second order homogeneous differential equations

A

auxiliary equation and then general solution depending on roots of auxiliary equation

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3
Q

method for second order non-homogeneous differential equations

A

complementary function and particular integral in the same form as f(x) or multiply by x or x^2 if in same form as CF

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4
Q

form of general solution for real unequal roots

A

y=Ae^ax+Be^bx

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5
Q

form of general solution for real equal roots

A

y=(Ax+B)e^ax

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6
Q

form of general solution for complex roots

m=a+/-bi

A

y=e^ax(Acosbx+Bsinax)

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7
Q

steps for Riemann sums

A
  1. divide domain into n strips of width Δx=b-a/n
  2. find grid points
  3. evaluate riemann sum

(could be left, right, upper or lower)

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8
Q

midpoint rule

A

Δx[f(x1bar)+…+f(xnbar)]

where Δx=(b-a)/n and x bar is midpoint of interval

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9
Q

trapezium rule

A

the average of the L and R Riemann sums

1/2(Ln+Rn)
=Δx/2[f(x0)+2f(x1)+…+2f(xn-1)+f(xn)]

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10
Q

simpson’s rule

A

use parabolae instead of straight lines
n must be even

consider consecutive pairs of intervals and approximate the integral over each pair

Δx/3(y0+4y1+2y2+4y3+2y4+…+2yn-2+4yn-1+yn)

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11
Q

general steps for approximate integration

A
  1. find Δx
  2. find x0,x1,…,xn
  3. (midpoint) x1bar, x2bar…
  4. f(x1), f(x2),… etc
  5. apply formula
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12
Q

function is continuous on an interval if…

A

continuous at every number in interval

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13
Q

function is differentiable at a if..

A

f’(a) exists

differentiable on an open interval if differentiable at every point

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14
Q

F is an anti derivative of f if

A

F’(x)=f(x) for all x

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15
Q

what form are integrals in for integration by substitution?

A

∫f(g(x))g’(x)

u=g(x) is a differentiable function, continuous on I

∫f(g(x))g’(x) dx = ∫f(u) du

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16
Q

limits in integration by substitution

A

change limits using expression for u and sub in current limits

limits are g(a) and g(b)

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17
Q

trigonometric integrals

A

manipulate integrand using trig identities

can use substitution in reverse by setting x=g(f) and obtain inverse substitution

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18
Q

integral on closed interval [-a,a], if f is even (i.e. f(-x)=f(x))

A

∫a/-a f(x)dx = 2∫a/0 f(x) dx

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19
Q

integral on closed interval [-a,a], if f is odd (i.e. f(-x)=-f(x))

A

∫a/-a f(x)dx = 0

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20
Q

integration by parts formula

A

∫uv’=uv-∫vu’

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21
Q

what is needed to split into partial fractions?

A

proper function
degree numerator < degree denominator

if not, denominator into numerator

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22
Q

4 different forms of partial fraction

A

distinct linear factors
repeated linear factors
irreducible quadratic factors
repeated irreducible quadratic factors

23
Q

distinct linear factors

A

A/ax+b + B/cx+d

24
Q

repeated linear factors

A

A/ax+b + B/(ax+b)^2

25
Q

irreducible quadratic factors

A

Ax+b/ax^2+bx+c

26
Q

repeated irreducible quadratic factors

A

Ax+b/ax^2+bx+c + Cx+d/(ax^2+bx+c)^2

27
Q

area between two curves y=f(x), y=g(x) and lines x=a, x=b

f(x)>/= g(x) for all x in [a,b]

A

A=∫a/b [f(x)-g(x)]dx

28
Q

area between two curves y=f(x), y=g(x) and lines x=a, x=b

f(x) < g(x)

A

A=∫a/b |f(x)-g(x)| dx

29
Q

volume: s is solid, lies between x=a and x=b.

if cross-sectional area of S in plane Px, through x and perpendicular to x=axis then V=

A

lim as n approaches infinity

∫ b/a A(x) dx

30
Q

solids of revolution

A

obtained by revolving a region about a lines

v=∫ b/a A(x) dx

where A is area of cross-section

31
Q

volume of revolution if cross -section is a disk

A

v=∫ b/a A(x) dx

A=pi(radius)^2

32
Q

volume of revolution if cross-section is a washer

A

v=∫ b/a A(x) dx

A=pi(router)^2-pi(rinner)^2

33
Q

volumes by cylindrical shells of revolution

rotating about y-axis, region under curve y=f(x), from a to b

A

v=∫b/a 2pix f(x) dx

=circumference.height.thickness

34
Q

volumes by cylindrical shells of revolution

rotating about x-axis, region under curve x=f(y), from c to d

A

v=∫b/a 2piy f(y) dy

35
Q

if f’ continuous on [a,b], length of curve is

A

L=v=∫b/a root(1+f’(x)^2 dx

(or root 1+ (dy/dx)^2 dx)

36
Q

differential of arc length

A

ds=root 1+(dy/dx)^2 dx

37
Q

arc length function

A

smooth curve equation y=f(x), s(x) is distance along curve from initial point P to Q

s(x) = ∫x/a root 1+ (f’t)^2 dt

38
Q

surface area of revolution

A

f +ve, continuous derivative, surface area by rotating y=f(x) about x-axis

s= ∫b/a 2piy ds

where ds= root 1+ (dy/dx)^2 dx

39
Q

what are parametric equations used for?

A

to describe curves not in the form y=f(x) i.e. fails vertical line test

40
Q

parametric equations

dy/dx=

A

dy/dt / dx/dt

41
Q

parametric area under y=F(x) from a to b, x=f(t), y=g(t)

t between alpha and beta

A

A=∫b/a F(x) = ∫beta/alpha g(t)f’(t) dt

42
Q

parametric arc length

A

L=∫beta/alpha root (dx/dt)^2+ (dy/dt)^2 dt

43
Q

parametric surface area of revolution

A

s=∫beta/alpha 2piy(t) root (dx/dt)^2+ (dy/dt)^2 dt

44
Q

limits of vector functions

A

take each component separately

make sure to sub point into original equation to get in terms of t

45
Q

d/dt [u(t)xv(t)] =

A

u’(t)xv(t) + u(t)xv’(t)

46
Q

unit tangent vector to space curve r(t) is

A

T(t) = r’(t)/|r’(t)|

47
Q

unit normal vector to space curve r(t) is

A

N(t)=T’(t)/|T’(t)|

48
Q

improper integral

A

interval is infinite or f has an infinite discontinuty.

49
Q

Type 1 improper integral

A

if ∫t/a f(x) dx exists for every t>/= a then

∫ infinity/a f(x) dx = lim as t appraoches infinity ∫t/a f(x) dx

same for negative infinity

50
Q

convergent

A

limit exists

51
Q

divergent

A

limit does not exist

52
Q

type 2 improper integrals

A

if f continuous on [a,b) and discontinuous at b

∫b/a f(x)dx=lim t –> b- ∫t/a f(x) dx

if f continuous on (a,b] and discontinuous at a

∫b/a f(x)dx=lim t –> a+ ∫b/t f(x) dx

53
Q

comparison theorem

A

if f(x) and g(x) continuous with f(x) >/= g(x)>/=0 for x>/=a

if ∫ infinity/a f(x) is convergent, ∫ infinity/a g(x) convergent

if ∫ infinity/a g(x) is divergent, ∫ infinity/a f(x) divergent