For the following exercises, Fourier’s law of heat transfer states that the heat flow vector F at a point is proportional to the negative gradient of the temperature; that is, F = − k ∇ T , which means that heat energy flows hot regions to cold regions. The constant k > 0 is called the conductivity , which has metric units of joules per meter per second-kelvin or watts per meter-kelvin. A temperature function for region D is given. Use the divergence theorem to find net outward heat flux ∬ s F ⋅ N d S = − k ∬ s ∇ T ⋅ N d S across the boundary S of D where k = 1 . 426. T ( x , y , z ) = 100 + e − x 2 − y 2 − z 2 ; D is the sphere of radius a centered at the origin.
For the following exercises, Fourier’s law of heat transfer states that the heat flow vector F at a point is proportional to the negative gradient of the temperature; that is, F = − k ∇ T , which means that heat energy flows hot regions to cold regions. The constant k > 0 is called the conductivity , which has metric units of joules per meter per second-kelvin or watts per meter-kelvin. A temperature function for region D is given. Use the divergence theorem to find net outward heat flux ∬ s F ⋅ N d S = − k ∬ s ∇ T ⋅ N d S across the boundary S of D where k = 1 . 426. T ( x , y , z ) = 100 + e − x 2 − y 2 − z 2 ; D is the sphere of radius a centered at the origin.
For the following exercises, Fourier’s law of heat transfer states that the heat flow vector
F
at a point is proportional to the negative gradient of the temperature; that is,
F
=
−
k
∇
T
, which means that heat energy flows hot regions to cold regions. The constant
k
>
0
is called the conductivity, which has metric units of joules per meter per second-kelvin or watts per meter-kelvin. A temperature function for region
D
is given. Use the divergence theorem to find net outward heat flux
∬
s
F
⋅
N
d
S
=
−
k
∬
s
∇
T
⋅
N
d
S
across the boundary
S
of
D
where
k
=
1
.
426.
T
(
x
,
y
,
z
)
=
100
+
e
−
x
2
−
y
2
−
z
2
;
D
is the sphere of radius
a
centered at the origin.
Quantities that have magnitude and direction but not position. Some examples of vectors are velocity, displacement, acceleration, and force. They are sometimes called Euclidean or spatial vectors.
Q2: Using the Laplace transform, find the solution for the following equation
y"" +y" = 6et + 6t + 6. Suppose zero initial conditions (y"" (0) = y"(0) = y'(0) = y(0) = 0).
1- Let A = {A1, A2, ...), in which A, A, = 0, when i j.
a) Is A a π-system? If not, which element(s) should be added to A to become a π-system?
b) Prove that σ(A) consists of the finite or countable unions of elements of A; i.c., A E σ(A) if and
only if there exists finite or countable sequence {n} such that A = U₁An (Hint: Let F be such
class; prove that F is a σ-filed containing A.)
c) Let p ≥ 0 be a sequence of non-negative real numbers with Σip₁ = 1. Using p₁'s, how do you
construct a probability measure on σ(A)? (Hint: use extension theorem.)
2- Construct an example for which P(lim sup A,) = 1 and P(lim inf An) = 0.
3. Let
f(z) =
sin (22) + cos (T2)
2(22+1)(z+1)
Compute f(z)dz over each of the contours/closed curves C1, C2, C3 and C4 shown
below.
Don't use any Al tool
Don't send the same
previous answer that
was Al generated
L
10
-c
x
show ur answer
pe
n and paper then take
Send ur answer in pe
n and paper don't rep
uted ur self down
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