Gradient Question: Why Does Direction Maximize Function?

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SUMMARY

The gradient vector of a function, represented as ∇f(x,y) = (∂f/∂x)i + (∂f/∂y)j, is always perpendicular to the level curves and surfaces of that function. This perpendicularity indicates that moving in the direction of the gradient maximizes the function's value, akin to ascending a hill directly rather than winding around it. The directional derivative, f_θ, can be expressed as ∇f · e_θ, where e_θ is the unit vector in the direction of angle θ. To find the direction that maximizes f, one must differentiate f_θ with respect to θ, leading to the conclusion that the angle θ for maximum increase aligns with the direction of the gradient.

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kidsasd987
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This is a bit counterintuitive to me that the gradient vector is always normal to the level curve
and the level surface.

lets say we have a function f(x,y)=z

then the gradient is,

f(x,y) partial derivative with respect to x*i +f(x,y) partial derivative with respect to y*j


what we actually get is,

dz/dx*i+dz/dy*j=grad_f(x,y)

then,

[(dz/dx*i)+(dz/dy)*j]/sqrt((dz/dx*i)^2+(dz/dy*j)^2)

this is always perpendicular to the level curve. But why does that direction always maximize the function?
 
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Think of going up a hill. You always have to go perpendicular to the level curve. You're not going to be winding around the side if you want the most direct route.
 
Another way of looking at it: if z= f(x, y) then the "directional derivative", f_{\theta}, the rate of change of f as you move in the direction that makes angle \theta with the positive x axis, is \nabla f\cdot \vec{e}_{\theta} where \vec{e}_{\theta} is the unit vector in that direction, which, in turn, is equal to \left(\frac{\partial f}{\partial x}\vec{i}+ \frac{\partial f}{\partial y}\vec{j}\right)\cdot \left(\vec{i}cos(\theta)+ \vec{j}sin(\theta)\right)= cos(\theta)\frac{\partial f}{\partial x}+ sin(\theta)\frac{\partial f}{\partial x}.

To maximize (or minimize) that with respect to \theta, take the derivative with respect to \theta, set it equal to 0 and solve for \theta. you will get
tan(\theta)= \frac{\frac{\partial f}{\partial y}}{\frac{\partial f}{\partial x}}
showing that \theta for the maximum is, indeed, the direction in which \nabla f points while the minimum is in the opposite direction.
 

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