update
This commit is contained in:
Vendored
BIN
Binary file not shown.
@@ -379,14 +379,14 @@ $$
|
||||
\alpha = \boldsymbol{z}^T\boldsymbol{x},
|
||||
$$
|
||||
|
||||
<p>which means that (using our previous example) we have</p>
|
||||
<p>which means that (using our previous example and keeping track of our definition of the derivative of a scalar) we have</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \boldsymbol{z}=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \frac{\partial \boldsymbol{z}^T\boldsymbol{x}}{\partial \boldsymbol{x}}=\boldsymbol{z}^T=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
$$
|
||||
|
||||
<p>Note that the resulting vector elements are the same for \( \boldsymbol{z}^T \) and \( \boldsymbol{z} \), the only difference is that one is just the transpose of the other.</p>
|
||||
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{y}} = \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T.
|
||||
$$
|
||||
|
||||
@@ -364,9 +364,14 @@ MathJax.Hub.Config({
|
||||
|
||||
<p>We list here some other useful relations we may encounter (recall that vectors are defined by boldfaced low-key letters)</p>
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{b}^T\boldsymbol{a})}{\partial \boldsymbol{a}} = \boldsymbol{b},
|
||||
\frac{\partial (\boldsymbol{x}^T\boldsymbol{a})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{a}^T\boldsymbol{x})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
|
||||
$$
|
||||
\frac{\partial tr(\boldsymbol{B}\boldsymbol{A})}{\partial \boldsymbol{A}} = \boldsymbol{B}^T,
|
||||
$$
|
||||
|
||||
@@ -537,16 +537,16 @@ $$
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
<p>which means that (using our previous example) we have</p>
|
||||
<p>which means that (using our previous example and keeping track of our definition of the derivative of a scalar) we have</p>
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \boldsymbol{z}=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \frac{\partial \boldsymbol{z}^T\boldsymbol{x}}{\partial \boldsymbol{x}}=\boldsymbol{z}^T=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
<p>Note that the resulting vector elements are the same for \( \boldsymbol{z}^T \) and \( \boldsymbol{z} \), the only difference is that one is just the transpose of the other.</p>
|
||||
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{y}} = \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T.
|
||||
@@ -715,7 +715,13 @@ $$
|
||||
<p>We list here some other useful relations we may encounter (recall that vectors are defined by boldfaced low-key letters)</p>
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{b}^T\boldsymbol{a})}{\partial \boldsymbol{a}} = \boldsymbol{b},
|
||||
\frac{\partial (\boldsymbol{x}^T\boldsymbol{a})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{a}^T\boldsymbol{x})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
|
||||
@@ -602,14 +602,14 @@ $$
|
||||
\alpha = \boldsymbol{z}^T\boldsymbol{x},
|
||||
$$
|
||||
|
||||
<p>which means that (using our previous example) we have</p>
|
||||
<p>which means that (using our previous example and keeping track of our definition of the derivative of a scalar) we have</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \boldsymbol{z}=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \frac{\partial \boldsymbol{z}^T\boldsymbol{x}}{\partial \boldsymbol{x}}=\boldsymbol{z}^T=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
$$
|
||||
|
||||
<p>Note that the resulting vector elements are the same for \( \boldsymbol{z}^T \) and \( \boldsymbol{z} \), the only difference is that one is just the transpose of the other.</p>
|
||||
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{y}} = \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T.
|
||||
$$
|
||||
@@ -739,9 +739,14 @@ $$
|
||||
|
||||
<p>We list here some other useful relations we may encounter (recall that vectors are defined by boldfaced low-key letters)</p>
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{b}^T\boldsymbol{a})}{\partial \boldsymbol{a}} = \boldsymbol{b},
|
||||
\frac{\partial (\boldsymbol{x}^T\boldsymbol{a})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{a}^T\boldsymbol{x})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
|
||||
$$
|
||||
\frac{\partial tr(\boldsymbol{B}\boldsymbol{A})}{\partial \boldsymbol{A}} = \boldsymbol{B}^T,
|
||||
$$
|
||||
|
||||
@@ -679,14 +679,14 @@ $$
|
||||
\alpha = \boldsymbol{z}^T\boldsymbol{x},
|
||||
$$
|
||||
|
||||
<p>which means that (using our previous example) we have</p>
|
||||
<p>which means that (using our previous example and keeping track of our definition of the derivative of a scalar) we have</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \boldsymbol{z}=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{x}} = \frac{\partial \boldsymbol{z}^T\boldsymbol{x}}{\partial \boldsymbol{x}}=\boldsymbol{z}^T=\boldsymbol{A}^T\boldsymbol{y}.
|
||||
$$
|
||||
|
||||
<p>Note that the resulting vector elements are the same for \( \boldsymbol{z}^T \) and \( \boldsymbol{z} \), the only difference is that one is just the transpose of the other.</p>
|
||||
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
<p>Since \( \alpha \) is a scalar we have \( \alpha =\alpha^T=\boldsymbol{x}^T\boldsymbol{A}^T\boldsymbol{y} \). Defining now \( \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T \) we find that</p>
|
||||
$$
|
||||
\frac{\partial \alpha}{\partial \boldsymbol{y}} = \boldsymbol{z}^T=\boldsymbol{x}^T\boldsymbol{A}^T.
|
||||
$$
|
||||
@@ -816,9 +816,14 @@ $$
|
||||
|
||||
<p>We list here some other useful relations we may encounter (recall that vectors are defined by boldfaced low-key letters)</p>
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{b}^T\boldsymbol{a})}{\partial \boldsymbol{a}} = \boldsymbol{b},
|
||||
\frac{\partial (\boldsymbol{x}^T\boldsymbol{a})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
$$
|
||||
\frac{\partial (\boldsymbol{a}^T\boldsymbol{x})}{\partial \boldsymbol{x}} = \boldsymbol{a}^T,
|
||||
$$
|
||||
|
||||
|
||||
$$
|
||||
\frac{\partial tr(\boldsymbol{B}\boldsymbol{A})}{\partial \boldsymbol{A}} = \boldsymbol{B}^T,
|
||||
$$
|
||||
|
||||
Binary file not shown.
+422
-410
File diff suppressed because it is too large
Load Diff
@@ -315,16 +315,16 @@ $\bm{z}^T=\bm{y}^T\bm{A}$, a vector of length $n$. We have then, using the defin
|
||||
\alpha = \bm{z}^T\bm{x},
|
||||
\]
|
||||
!et
|
||||
which means that (using our previous example) we have
|
||||
which means that (using our previous example and keeping track of our definition of the derivative of a scalar) we have
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial \alpha}{\partial \bm{x}} = \bm{z}=\bm{A}^T\bm{y}.
|
||||
\frac{\partial \alpha}{\partial \bm{x}} = \frac{\partial \bm{z}^T\bm{x}}{\partial \bm{x}}=\bm{z}^T=\bm{A}^T\bm{y}.
|
||||
\]
|
||||
!et
|
||||
|
||||
Note that the resulting vector elements are the same for $\bm{z}^T$ and $\bm{z}$, the only difference is that one is just the transpose of the other.
|
||||
|
||||
Since $\alpha$ is a scalar we have $\alpha =\alpha^T=\bm{x}^T\bm{A}^T\bm{y}$. Defining now $\bm{z}=\bm{x}^T\bm{A}^T$ we find that
|
||||
Since $\alpha$ is a scalar we have $\alpha =\alpha^T=\bm{x}^T\bm{A}^T\bm{y}$. Defining now $\bm{z}^T=\bm{x}^T\bm{A}^T$ we find that
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial \alpha}{\partial \bm{y}} = \bm{z}^T=\bm{x}^T\bm{A}^T.
|
||||
@@ -477,9 +477,15 @@ or as
|
||||
We list here some other useful relations we may encounter (recall that vectors are defined by boldfaced low-key letters)
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial (\bm{b}^T\bm{a})}{\partial \bm{a}} = \bm{b},
|
||||
\frac{\partial (\bm{x}^T\bm{a})}{\partial \bm{x}} = \bm{a}^T,
|
||||
\]
|
||||
!et
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial (\bm{a}^T\bm{x})}{\partial \bm{x}} = \bm{a}^T,
|
||||
\]
|
||||
!et
|
||||
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial tr(\bm{B}\bm{A})}{\partial \bm{A}} = \bm{B}^T,
|
||||
|
||||
Reference in New Issue
Block a user