|
(t, x, y, z), t > 0).
, -b2 < h <
-c2, -a2 < z < -b2.
. Also, labeled null set.
Y in a category (PL) is an
inxlusion map (PL) e:E
X s.t. (composition)
f o e= g o e; any other map with the same property fits with the
inclusion map and an identity map in a commutative diagram (PL). The equalizer is a
monomorphism (PL), unique up to isomorphism (PL). In the category of sets,
the equalizer is given by the set, E = {e e x: f(x) =
g(x)} and by the above inclusion map. The dual (PL) is coequalizer.
R
, then the essential supremum is least number, n,
s.t. the set, {x: f(x) > n}, has measure zero (PL). If no such
number exists -- as for f(x) = 1/x on open set, (0, 1)
, then the essential supremum is
. The essential supremum of the
absolute value of a function, ||f||
provides the norm for L-infinity-space.
y; so that the product rotation
is r11 = cos y cos
f - cos q sin y sin f
, r21 = cos y cos f + cos q sin y sin f, r13 = sin y sin
q, r21 = - sin y
cos f - cos q sin f
cos y, r22 = - sin y cos f + cos q sin fcos y, r23 =
cos y sin q, r31
= sin q sin f,
r32 = - sin q cos f, r33 = cos q. For computational purposes,
instead of Euler angles, the general rotation is obtained via the Euler
parameters (PL).
j
k
i, and ij =
k, jk = i, ki = j. Using the parameters, the rotation formula becomes: r' = r(e02 - e
12 - e22 - e
3) + 2e(e · r) + (r X normal)sinf.
S
n=0En
tn/n!. The Euler polynomials are related to the Bernoulli
numbers (PL), and satisfy the identities: En(x + 1) + E
n(x) = 2xn.
df is path-independent, requring that
df = Dxf dx + Dyf dy.
, meaning
"for at least one _". PL universal quantifier.
n(n - 1)(n- 2)(n - 3)...(2)(1). It arises from the equation y =
ln x, for natural logaritm, "ln" (PL). Remarkably, the exonential function
equals its derivative, that is, Dxex = ex
. It "passes to the limit" so nicely that it is used as a comparator in testing
convergence (PL) of other series (PL). A base (PL) for exponentiation
(PL) can be used other than e, but easily related to it. Thus, bx = ex ln b.
n(n - 1)(n- 2)(n - 3)...(2)(1)
, and 0! = 1!
1.
b + (-1)p a
db
, where a is a k-form and
is the wedge product. The exterior derivative is a (k + 1)-
form. Thus, for a k-form, w1 =
b1 dx 1 + b2 dx3, the exterior derivative is
dw1 = db1
dx1 + db2
dx2.