Applied Stuff - the beg. of relativistic applied

mass m, time interval dt, small angle dw, speed of light c
-0.5m*v(dw/dt) + E - mc^2 = 0
-0.5m/c*v(dw/dt) + E/c - mc = 0
-0.5m/c*v(dw/dt) + E/c = mc
E = m*g[r]
-0.5m/c*vdw/dt + m*g[r]/c = mXc

equation still works with kinetic energy formula
-0.5m*v(dx/dt) + E - mc^2 = 0
-0.5m/c*v(dx/dt) + E/c - mc = 0
-0.5m/c*v(dx/dt) + E/c = mc
E = m*g[r]
-0.5m/c*v(dx/dt) + m*g[r]/c = mXc
whatever teeheehee!

speed make by deriving m, or setting m=1.
-0.5v/c*dw/dt + g[r]/c = c
-(1/2)v/c*dx/dt + g[r]/c = c
"Argh!" You say later on! E/c^2 = m, is better however. As we saw previously.
-0.5E/c*v(dx/dt) + E/c*g[r] = E/c
-0.5v(dx/dt) + g[r] = 1
-0.5v(dx/dt)/[r] + g = 1/[r]
g = 1/[r] + 0.5v(dx/dt)/[r]
Where g is constant acceleration on a surface above a point mass. It is noticed
that there is a parabolic equation however!
0 = 0.5v(dx/dt) - g[r] + 1
Therefore! r=x
0.5v^2 - g*x + 1  = 0
(dx/dt)^2 = 2g*x - 2
dx/dt = [2(g*x - 1)]^0.5

time maker
-0.5/c*dw/dt + g[r]/(vXc) = c/v
-0.5/c*dw/dt + g[r]/(vXc) = c(x)/t
-0.5/c*dw/dt + g[r]/(vXc) = c(cos[w])/t
0 = -(1/2)v/c*dx/dt + g[r]/c/v + 0.5/c*dw/dt - g[r]/(vXc)
It is either small angle or small line. It is still a tiny number!
-(1/2)v*dx/dt + g[r]*v + 0.5dw/dt - g[r]/v = 0
0.5dw/dt = (1/2)v*dx/dt

acceleration measurer
Huh...
F = m*a
a = d(v)/dt
a/t = 1/t*d(v)/dt
a/t = 1/t*d(v)/dt
1/t turns into 1/(space)
a/t = 1/(b)[60 things for 1 counting]^n*d(v)/dt
a/x = t/(b)[2*2*3*5]^nd(v)/dt
C = t/(b)[2^n*2^n*3^n*5^n]d(v)/dt
C = t/(b)[2^n*2^n*3^n*5^n]d(v)/dt
F/x = m*t/(b)[2^n*2^n*3^n*5^n]d(v)/dt
-F*x = m*a*x
wha...? what is C? 'a' is a quantity that varies. It is this! C = da/X
b is now x, our distance. There are many things and you must discern between them
to count. Ergo, you have seperation and distance. X is our large space within which
we count the b things.
da*dt/X = t/(x)[2^n*2^n*3^n*5^n]d(v)/dt
Total time taken, T, by travelling object over distance X.
da*dt/X = T/[2^n*2^n*3^n*5^n]d(v)/dt
da(x)dt = X*T/[2^n*2^n*3^n*5^n]d(v)/dt
We leave this as is for now since integrating it will give you trouble.
~da(x)dt huh?

space create
+g[r] = c(vXc)/v + 0.5(vXc)/c*dw/dt
With F = G*mXM/r^2 as G*mXM/x^2 = m*d(v)/dt
GXM/r^2 = d(v)/dt

With SPACE CREATE we return to acceleration measurer!

da(x)dt = X*T/[2^n*2^n*3^n*5^n]GXM/r^2
~rda~rdt(x)/X/T/(GXM) = [2^n*2^n*3^n*5^n]
integrating
0.25(r^2)(r^2)/x/X/T/(GXM) = [2^n*2^n*3^n*5^n]
0.25(r^4)/x/X/T/(GXM) = [2^n*2^n*3^n*5^n]
now we have machine!

Now I make temperature sensor
The heat equation, with point U=u(x,y,z,time) that is agitated
pU/pt - alpha*Laplacien(U) = 0
where p is partial derivative of position of point U
~pU = ~alpha*Laplacien(U)pt
integrating
U = alpha*Laplacien(U)t
where L = density times specific heat capacity
U = k/L*Laplacien(U)t
U*L/k/Laplacien(U) = t
U/L/Laplacien(U)t = k [W/(l*K)]
where k = energy, E, (in watts) over length, x, and temp., K, in kelvins
U/L/Laplacien(U)t = E/x*K
Power equation
U/L/Laplacien(U)x*K = E/t
returning to initial equation we find that
-0.5m*v(dw/dt) + (U/L/Laplacien(U)t(x*K)) - mc^2 = 0
small angle dw is now small length dx
U/L/Laplacien(U)t(x*K) = 0.5m*v(dx/dt) + mc^2
K/Laplacien(U) = L/U*0.5xXm*v(dx/dt)/t + L/U*xXmc^2/t
K = xXm*L[0.5v(dx/dt) + c^2]Laplacien(U)/t/U
interpreting equation
m, mass makes temp increase
x, uni-dimensional point makes temp increase
L = densityXHeat capacity of material, such that
density and specific heat capacity makes temp increase
v, speed makes temp increase
dx/dt, makes temp either increase when >1 or decrease when <1
t, time makes temp decrease
x, measured point makes temp increase
Laplacien(U)
t, time when <1, will increase temperature
U, having position of a point in time decreases temperature when ||U||>1