June 14, 20XX

As the fourteenth day of the Battle of Mushroom Raceways dawns upon us, chaos engulfs the battlefield like never before. The once serene landscape has been transformed into a nightmarish battleground, where heroes and villains clash in a desperate struggle for supremacy. The air is thick with tension, and the deafening sounds of explosions and clashes reverberate through the air.

Mario, Sonic, Luigi, Shadow, and Yoshi stand at the forefront, their determined expressions mirroring the gravity of the situation. They face their greatest adversary yet: the formidable Metallix. This robotic menace, imbued with incredible power, towers over our heroes, casting an ominous shadow across the war-torn terrain. Its glowing red eyes pierce through the chaos, exuding an aura of malevolence.

The clash begins with a burst of energy as Mario and Sonic launch themselves at Metallix simultaneously. Their agility and speed are unmatched, their movements blurring in a flurry of punches and kicks. Luigi and Yoshi, not to be outdone, join the fray, using their unique abilities to unleash devastating attacks upon their metallic foe. Shadow, with his dark and mysterious aura, provides the element of surprise, launching precise strikes aimed at Metallix's weak points.

The battlefield resembles a maelstrom of colors and flashing lights as the clash intensifies. The ground beneath us trembles with each explosive impact, scattering debris and causing the once-solid roadways to crumble. The chaos is disorienting, yet our heroes remain focused, fueled by their unwavering determination to protect this planet from the clutches of evil by King Bowser and Dr. Eggman with their forces and allies.

Meanwhile, a separate confrontation takes place nearby, drawing attention amidst the chaos. Robo Mario, a mechanical replica of Mario, squares off against Mecha Mario, another doppelgänger created with malicious intent. The two robotic counterparts clash with relentless force, each mirroring the other's movements flawlessly. It is a battle of wits and precision, where a single misstep can lead to catastrophic consequences.

The din of clashing metal and the eruption of energy beams create a symphony of destruction that reverberates throughout the battlefield. The very fabric of reality seems to warp and bend under the weight of this epic clash between heroes and villains. As spectators to this incredible spectacle, one can only marvel at the determination and bravery exhibited by these iconic characters.


Math Notes: (filled with academic musings)

Finding the tangent

y=-x^3 + 8x^2 - 20x + 14 at (2,-2)

dy/dx or slope (m) = -3x^2 + 16x - 20 at (2,-2)

m= -3(2)^2 + 16(2) - 20

m=0 or y'=0

y=mx+b

y=(0)x+b

y=(0)2-2

b=-2

Answer: y=-2

...

y= 6 / x^2+2 at (3, 6/11)

dy/dx = (x^2 + 2) d/dx(6) - (6) d/dx(x^2+2) / (x^2 + 2)^2

dy/dx = (x^2 + 2) (0) - (6) (2x+0) / (x^2 + 2)^2

dy/dx = (3^2 + 2) (0) - (6)(2 times 3+0) / (3^2 + 2)^2

dy/dx: m=-36/121

y=mx+b

y=(-36/121)x+b

(3, 6/11)

6/11=(-36/121)(3)+b

174/121=b

y=-36/121x + 174/121

...

y=-2sin(x) at (0,0)

dy/dx=-2cos(x)

m=-2cos(0)

m=0

-2cos(0)

=-2(1)

m=-2

y=(-2)x+b

y=(-2)(0)+b

0=(-2)(0)+0

b=0

y=(-2)x+0

...

y=(2x-4)^1/3 at (-2,-2)

dy/dx=1/3 (2x-4)^1/3-1

f'(x)=f(g(x)) Chain Rule

1/3 (2x-4)^1/3 - 1 (2)

dy/dx=1/3 (2x-4)^-2/3 (2)

(-2,-2)

x=-2

dy/dx=1/3 (2(-2)-4)^-2/3 (2)

dy/dx=1/6

m=1/6

y=(1/6)x+b

(-2)=(1/6)(-2)+b

b=-7/3

y=(1/6)x - 7/3

...

y= -3sin(x) at (0,0)

dy/dx=-3sin(x)

m=-3cos(0)

m=0

cos(0)=1

So: -3cos(0)

=-3(1)

m=-3

y=(-3)x+b

y=(-3)(0)+b

b=0

y=(-3)x+0

...

y=(2x-4)^1/4 at (-2,-2)

y=(3x-5)^1/4 at (-3,-3)

dy/dx=1/4(3x-5)^1/4-1

f'(x)=f(g(x)) chain rule

dy/dx=1/4(3x-5)^1/4 - 1 (3)

(-3,-3)

dy/dx=1/4(3(-3)-5)^1/4 - 1 (3)

dy/dx=1/4(3(-3)-5)^-5/4 (3)

Domain Error

...

y=(3x-5)^1/2 at (-3,-3)

dy/dx = 1/2(3x-5)^1/2-1

f'(x)=f(g(x)) chain rule

dy/dx=1/2(3x-5)^-1/2 (3)

dy/dx=1/2(3(-3)-5)^-3/2(3)

Domain Error

...

Mean Value Theorm

Continious [a,b] vs (a,b)

f'(c)=f(b)-f(a) / b-a

mtan=msec

m=y2-y1 / x2-x1

f(x)=y

f(b)=y2

f(a)=y1

...

f'(c)= f(b)-f(a) / b-a

f(x)=2x^3 + x^2 + 7x - 1 on [1,6]

f(a)=2(1)^3 + (1)^2 + 7(1) - 1

f(a)=9

f(b)=2(6)^3 + (6)^2 + 7(6) - 1

f(b)=509

509-9 / 6-1 = 100

f'(c)=100

Derivative

dy/dx = f'(x) = 6x^2 + 2x + 7

100=6x^2 + 2x + 7

0=6x^2 + 2x - 93

-b+/- square root b^2 - 4(a)(c) / 2(a)

-2+/- square root 2^2 - 4(6)(-93) / 2(6)

=3.77... and -4.11...

x=3.77...

Plug in the x to the f(x)'s x

=(3.77... , 147.15...)

...

f(z)=4z^3 - 8z^2 + 7z - 2 on [2,5]

f(a)=4(2)^3 - 8(2)^2 + 7(2)-2

f(a)=12

f(b)=4(5)^3 - 8(5)^2 + 7(5) - 2

f(b)=333

333-12 / 5-2 = 321/3 = 107

f'(c)=107

dy/dx=f'(z)=12z^2 - 16z + 7

107=12z^2 - 16z + 7

0=12z^2 -16z - 100

Since difficult to factor: -b+/- sqaure root b^2 - 4(a)(c) / 2(a)

-(-16)+/- square root (-16)^2 - 4(12)(-100) / 2(12)

x= 3.63...

x=3.63...

y=4(3.63...)^3 - 8(3.63...)^2 + 7(3.63...) - 2

y=109.26...

(3.63... , 109.26...)

...

1) Find the derivative set = 0. Solve for x

2) Create a number line and plug in points close to the extremas to determined if the extremas are relative with minimums and maximums.

3) Plug in the endpoints as well as the relative extremas.

4) Determine the absolute extrema by carrying y-values

f(x)=x^2 - 4x + 9; [1,4]

x=2

f(1)=1^2 - 4(1) + 9

1-4+9=6

f(2)=2^2 - 4(2) + 9

4-8+9=5

f(4)=4^2 - 4(4) + 9

16-16+9=9

f(x)=x^2-4x+9

f'(x)=2x-4=0

0=2(x-2)

x=2

Number line: Before 2 has negative range, after 2 has positive range

(1,6)

(2,5): absolute min

(4,9): absolute max

...

y=-x^3 + x^2 - 3; [-1,1]

y'=-3x^2 + 2x

0=-3x^2 + 2x

x(-3x+2)

x=0, x=2/3

f(-1/3)=-3(-1/3)^2 + 2(-1/3)

f(-1/3)=-1

f(1)=-1

f(1/3)= -3(1/3)^2 + 2(1/3) = 1/3

Max: (-1,-1)

(2/3, -2.85...)

Min: (0,3), (1-3)