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sphere eqn
direction angles
v = <a, b, c>
a → α
scalar projection (b onto a)
*magnitude of b that falls over a
vector projection (b onto a)
*captures scalar projection as well as direction
limit of a vector
dot product
cross product
a x b = area of parallelogram
|a • (b x c)| = area of parallelepiped
vector eqn
parametric eqns (vector)
v = <a, b, c>
v: parallel to actual vector, defines direction
symmetric eqns (vector)
2-point vector eqn
r0 + v = r1
v: vector connecting points r0 & r1
scalar plane eqn
P0 = <x0, y0, z0>
n = <a, b, c>
linear plane eqn
d = -(ax0 + by0 + cz0)
ellipsoid
cone
elliptic paraboloid
hyperbolic of one sheet
hyperbolic paraboloid
hyperboloid of two sheets
unit tangent vector
derivative of a vector
derivative of cross & dot product
integral of a vector
arc length
curvature
unit normal
unit binormal
B(t) = T(t) x N(t)
acceleration (tangent & normal)
partial derivative
b = constant
derivative notation
Clairaut’s thm
If fxy & fyx are continuous on D
fxy(a, b) = fyx(a, b)
True for most functions
plane eqn
a = -A/C
b = -B/C
total differential
chain rule (multivariable)
intermediate variables: ???
implicit differentiation??? (multivariable)
implicit function theorem?
directional derivative
rate of change of a multivariable function along some unit vector u
u = <a, b>
gradient vector
shows direction of fastest increase
tangent plane (symmetric eqns)
critical point (multivariable)
fx and fy = 0
fx or fy DNE
SDT
D > 0:
fxx(a, b) > 0
Local minimum
fxx(a, b) < 0
Local maximum
D < 0:
no max/min
EVT (multivariable)
if f is continuous on closed, bounded D:
Both an absolute max & min exist within D
lagrange multiplier
Find all values of lambda satisfying:
∇f(x0, y0, z0) = λ∇g(x0, y0, z0)
g(x, y, z) = k
Evaluate f @ all points
Greatest f is maximum, smallest is minimum
average value (multivariable)
double integral
general regions (double integral)
type 1: between 2 continuous functions of x
type 2: between 2 continuous functions of y
double integral (polar)
*similarity: r dθ = arc length → “area” dA = r dr dθ
lamina mass
COM (multivariable)
moment of inertia (Ix, Iy, I0)
I0 + Ix + Iy
radius of gyration
average distance from the axis of rotation (R)
R = sqrt(I/m)
If all mass was concentrated R distance from the axis, I = mR2 regardless of shape/distribution
surface area (multivariable)
triple integral
yields bound volume if f(x, y, z) = 1
general regions (triple integral)
type 1:
between graphs of 2 continuous f(x, y) functions
region D projected from xy-plane
type 2:
between graphs of 2 continuous f(y, z) functions
region D projected from yz-plane
type 3:
between graphs of 2 continuous f(x, z) functions
region D projected from xz-plane
moments of inertia (3 axes)
moments (3 axes)
x̄ = Myz/m
ȳ = Mxz/m
z̄ = Mxy/m
cylindrical coords
(θ, r, z)
spherical coords
(ρ, θ, Φ)
Jacobian
x = g(u, v)
y = h(u, v)
vector fields
assigns each point on the coordinate plane with a vector F(x, y) or F(x, y, z)
conservative vector field
F is conservative if some f exists where:
F = ∇f
line integral (standard)
line integral (x’(t))
line integral (short form)
P integration only considers value change over changes in x
Q integration only considers value change over changes in y
work done (line integral)
T = unit tangent on C
Fundamental theorem for line integrals
line integrals of conservative vector fields only require values of f @ C’s endpoints!
test for conservative vector field
F(x, y) = P(x, y)i + Q(x, y)j
ONLY true in a simple region
Green’s thm
true if P & Q have continuous partial derivatives on D
Area (region D around closed line integral)
curl
F = Pi + Qj + Rk
measures rotation in a vector field
curl(∇f)
implies conservative vector fields also have no curl
true if second-order partial derivatives are continuous
divergence
measures the rate at which vectors move away from a point
div curl
true if F has continuous second-order partial derivatives
second vector form of green’s thm
parametric equations of surface S
surface of revolution
surface area/ surface integral
can be used for COM or moments of inertia
vector surface integrals
Stokes’ thm
Divergence thm