And there are never really endings, happy or otherwise. Things keep going on, they overlap and blur, your story is part of your sister’s story is part of many other stories, and there is no telling where any of them may lead. Everything turns in circles and spirals with the cosmic heart until infinity.
Recall that implicit differentiation is commonly used to find derivatives of functions defined implicitly or to find derivatives of functions that cannot be explicitly solved for one variable, y = f(x), dy = f’(x)dx, e.g., y = sin-1(x) ⇒ x = sin(y) ⇒ dx = cos(y)dy ⇒ $\frac{dy}{dx}=\frac{1}{cos(y)}=\frac{1}{\sqrt{1-x^2}}$
In multivariable Calculus, The total differential of a multivariable function f(x1, x2, ···,xn) is an expression that describes or encodes how a small change in each of its variables affects the function’s value. It is denoted by df and is defined as follows:df = $\frac{\partial f}{\partial x}d_x+\frac{\partial f}{\partial y}d_y+\frac{\partial f}{\partial z}d_z = f_xdx + f_ydy +f_zdz.$
It describes how the function changes as you move along an infinitesimal displacement in each of its variables, hence providing information about the rate of change of the function in each direction Besides, provides an approximation for small variations Δx, Δy, Δz, so Δf ≈ fxΔx + fyΔy + fzΔz.
The Chain Rule for multivariable functions is a fundamental concept in calculus that allows us to compute the derivative of a composite function. It states that if we have a function f(x, y, z) where x = x(t), y = y(t), and z = z(t) are functions of another variable t, then the derivate of f with respect to t is given by $\frac{df}{dt} = f_x\frac{dx}{dt} +f_y\frac{dy}{dt}+f_z\frac{dz}{dt}$.
Proof. (2 versions)
Version. df = $f_xdx + f_ydy +f_zdz,$ where x = x(t), y = y(t), and z = z(t) are functions of another variable t⇒ dx = x’(t)dt, dy = y’(t), dz = z’(t)dt ⇒ df = $f_xdx + f_ydy +f_zdz = f_xx’(t)dt + f_yy’(t)dt +f_zz’(t)dt$ ⇒[By dividing by dt] $\frac{df}{dt} = f_x\frac{dx}{dt} +f_y\frac{dy}{dt}+f_z\frac{dz}{dt},$ (The Chain Rule).
Version. Δf ≈ $f_xΔx + f_yΔy +f_zΔz$⇒[By dividing by Δt] $\frac{Δf}{Δt} = \frac{f_xΔx + f_yΔy +f_zΔz}{Δt} = f_x\frac{Δx}{Δt} + f_y\frac{Δy}{Δt} + f_z\frac{Δz}{Δt}⇒$ as Δt → 0, the approximation becomes an equality and we get the Chain Rule again, $\frac{df}{dt} = f_x\frac{dx}{dt} +f_y\frac{dy}{dt}+f_z\frac{dz}{dt}.$
Let’s apply the Chain Rule, $\frac{dw}{dt} = 2xy\frac{dx}{dt} + x^2\frac{dy}{dt} + \frac{dz}{dt} = 2te^t + t^2e^t+cos(t)$.
Another way of seeing it is as follows, w(t) = x2y+z = t2et + sin(t) ⇒ $\frac{dw}{dt} = 2te^t+t^2e^t+cos(t)$, that is obviously the same answer.
In particular, let f = uv, where u = u(t) and v = v(t) ⇒ $\frac{d(uv)}{dt}=f_u\frac{du}{dt}+f_v\frac{dv}{dt} = v\frac{du}{dt}+u\frac{dv}{dt}$, and we get the tradition Chain Rule.
Similarly, let g = u⁄v where u = u(t) and v = v(t) ⇒$\frac{d(u/v)}{dt} =f_u\frac{du}{dt}+f_v\frac{dv}{dt} = =\frac{1}{v}\frac{du}{dt}+\frac{-u}{v^2}\frac{dv}{dt} = \frac{u’v-v’u}{v^2}$, that is, the quotient rule.
w = f(x, y) where x = x(u, v) and y = y(u, v)
We already know that $dw = f_xdx +f_ydy = f_x(x_udu +x_vdv) +f_y(y_udu +y_vdv) =$[Collecting terms] $(f_xx_u+f_yy_u)du + (f_xx_v + f_yy_v)dv$ ⇒ $\frac{\partial f}{\partial u} = f_xx_u+f_yy_u, \frac{\partial f}{\partial v} = f_xx_v + f_yy_v$, that is, $\frac{\partial f}{\partial u} = \frac{\partial f}{\partial x}\frac{\partial x}{\partial u}+\frac{\partial f}{\partial y}\frac{\partial y}{\partial u}, \frac{\partial f}{\partial v} = \frac{\partial f}{\partial x}\frac{\partial x}{\partial v}+\frac{\partial f}{\partial y}\frac{\partial y}{\partial v}$
$\frac{\partial f}{\partial r} = \frac{\partial f}{\partial x}\frac{\partial x}{\partial r}+\frac{\partial f}{\partial y}\frac{\partial y}{\partial r} = f_xcos(θ) + f_ysin(θ)$