Easy proof of Why del(phi) is normal to a surface?

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In a 3D space defined by the function f(x,y,z) = 0, a unit vector normal to the surface at point (a,b,c) is expressed as ∇f(a,b,c) divided by the modulus of ∇f(a,b,c). The discussion highlights that the derivative Dₕ in the direction of a tangent vector is zero, indicating that ∇f is perpendicular to any tangent vector on the surface. Participants clarify that dividing ∇f by its length yields a unit normal vector. The importance of understanding the relationship between the gradient and the surface is emphasized, particularly through the use of the chain rule for differentiation. The conversation concludes with a focus on the mathematical principles underlying the normal vector's definition.
cpfoxhunt
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Homework Statement



Prove that for a 3d space s, defined by a function f(x,y,z) = 0 , a unit vector normal to surface at the point (a,b,c) is given by \nablaf(a,b,c) / modulus of \nablaf(a,b,c)

(Apologies for the bad use of latex)

Homework Equations



None really

The Attempt at a Solution



I can only seem to gesture at this - it was given us as a definition. I know that d(phi)/ds where phi is a surface and s is a distance = \nabla(Phi).A , and that surely if a is tangential the LHS is equal to zero, but I'm a bit stuck from there and not sure if I've used things I need to prove. Its only a few marks, but is bugging me.

Any help is greatly appreciated,
Cheers
Cpfoxunt
 
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Are you aware that D_{\vec{v}}\phi= \nabla\phi\cdot\vec{v}, where D_{\vec{v}} is the derivative in the direction of the unit vector \vec{v}? From that, it follows that if \vec{v} is tangent to a "level surface" \phi= constant, then D_{\vec{v}}\phi= \nabla\phi\cdot\vec{v}= 0. That is, \nabla\phi is perpendicular to any tangent vector and so to the surface itself.
 
I am aware of that (and now see why its important). That was what i was trying to get at with my attempt. But I'm still not quite happy - it doesn't explain the unit vector evaluated at (a,b,c), and I feel like I should try to gesture at why D(phi) = del(phi).V ?
 
I don't understand what you mean by "explain the unit vector". If you recognize that \nabla \phi is perpendicular to the surface, then of course dividing by its own length will give a unit vector in that direction.

As for why D_{\vec{v}}\phi= \nabla\phi\cdot\vec{v}, a unit vector can always be written in the form a\vec{i}+ b\vec{j}+ c\vec{k} where, of course, \sqrt{a^2+ b^2+ c^2}= 1. We can write a line in that direction as x= x_0+ at, y= y_0+ bt, and z= z_0+ bt. So \phi(x,y,z) in that direction is \phi( x_0+ at, y_0+ bt, z_0+ ct). Differentiate that with respect to t (using the chain rule) and see what you get.
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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