Calculating the Gradient of a Complex Exponential Function

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The discussion focuses on calculating the gradient of the complex exponential function e^{i\vec{k}\cdot \vec{r}}. The solution is confirmed to be \nabla e^{i\vec{k}\cdot \vec{r}} = i\vec{k} e^{i\vec{k}\cdot \vec{r}}, with a breakdown of the function into its components. Participants explore different approaches, including using the theorem \nabla f(r) = \frac{df}{dr}\nabla r, but some express confusion about its relevance in this context. The alternative method suggested involves treating the function as a composition, applying the chain rule with f(g) = e^g and g(\vec{r}) = i \vec{k} \cdot \vec{r}. Ultimately, the discussion emphasizes the importance of correctly applying mathematical principles to arrive at the solution.
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Homework Statement


Calculate \nabla e^{i\vec{k}\cdot \vec{r}}

Homework Equations


\nabla f(r)=\frac{df}{dr}\nabla r=\frac{df}{dr}\frac{\vec{r}}{r}

The Attempt at a Solution


I have a problem. I know result
=\nabla e^{i\vec{k}\cdot \vec{r}}=i\vec{k} e^{i\vec{k}\cdot \vec{r}}
 
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This problem is much clearer when broken up componentwise:
##e^{i \vec k \cdot \vec r } = e^{i (k_x x + k_y y + k_z z) } ##
Where ##\vec k = k_x \hat x + k_y \hat y + k_z \hat z ## and ##\vec r = x \hat x + y \hat y + z \hat z##
 
Yes but for that way we need a lot of time. Perhaps
\nabla=\sum_w\vec{e}_w\frac{\partial}{\partial x_w}
e^{i \vec{k}\cdot \vec{r}}=e^{i\sum_q k_q x_q}
but I get a problem with this sums. Maybe
\sum_w\vec{e}_w\frac{\partial}{\partial x_w}e^{i\sum_q k_q x_q}=
=\sum_w\vec{e}_we^{i\sum_q k_q x_q}(\frac{\partial}{\partial x_w}i\sum_q k_q x_q)=
=e^{i\vec{k}\cdot \vec{r}}i \sum_w \vec{e}_w k_{w}=
=i\vec{k}e^{i\vec{k}\cdot \vec{r}}

but again I did not use theorem
\nabla f(r)=\frac{df}{dr}\nabla r
 
LagrangeEuler said:
but again I did not use theorem
\nabla f(r)=\frac{df}{dr}\nabla r
let ##f(\vec r) = e^{ik_x \hat x +ik_y \hat y+ik_z \hat z}## and ##\vec r = ik_x \hat x +ik_y \hat y+ik_z \hat z = i \vec k \cdot \vec r##
then use the theorem.
 
I think that "relevant equation",
\nabla f(r)=\frac{df}{dr}\nabla r=\frac{df}{dr}\frac{\vec{r}}{r},
is not that relevant here:
e^{i\vec{k}\cdot \vec{r}}\neq f(r) since r = (x^2 + y^2 + z^2)^{1/2}.

Rather,
\nabla f(g(\vec r))=\frac{df}{dg}\nabla g(\vec r)
with
f(g) = e^g and g(\vec r) = i \vec k \cdot \vec r.
 
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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