"微分係数"の翻訳 英語に:


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微分係数 - 翻訳 :

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アルゴリズムだ それとニューラルネットワークの コスト関数の偏微分係数を 計算する方法
So that's the back propagation algorithm and how you compute derivatives of your cost function for a neural network.
2 番目の関数の微分 g1 y 2 番目の関数の微分は
So plus f1 of x, that's just the first function, times the derivative of the second function.
この係数の半分は 何ですか その係数の半分はー 2 です
You literally just look at this coefficient right here, and you say, OK, well what's half of that coefficient?
この係数の半分をとり この係数は 6 です 半分をは 3で
When we complete the square, we just take half of this coefficient.
ここでは 関係ありません 斉次微分方程式
But the application here, at least I don't see the connection.
これは変数分離形微分です これは 副ー微分方程式のようなもので
And this is actually a separable differential equation in and of itself.
この微分の導関数です 皆さんが微分積分の微分を見たことがあるか定かではありませんが
So, let's see what this, this equation will do.
この係数の半分をとり
Let's do that.
微分
Differentiation
μ x dμ dx  x これは変数分離形微分です
So we could write mu of x is equal to d, the derivative of mu with respect to x, times x.
xの関数のμ は yに関係ないので 定数と見なされます yに関する偏微分を取ると
Well, if we're taking the partial with respect to y here, mu of x, which is only a function of x, it's not a function of y, it's just a constant term, right?
この係数の半分は ー 2の半分で
Now let's go to the y terms.
積分の係数を0 004とします
Let's implement this in our code.
微分したら2xになります x 2をxで微分した導関数は2xになり
In general, the derivative with respect to x of X 2 plus any constant, any constant, is going to be equal to 2X.
微分を加えます 最初の関数 f1 x に
Now you add that to the derivative of the second function times the first function.
係数
Modulus
あらゆる点で微分可能な関数は連続関数です
A function that is differentiable everywhere is continuous.
微細構造定数
Fine Structure Constant
diff crosstrack errorという微分的な 変数を作りました
Here is my solution.
微分方程式は 未知の関数とその導関数に関する
What is a differential equation?
微積分や
You've already dealt with vectors.
変数分離形微分方程式は 積分の一般解の逆です 一般的に 微分方程式の面白い点けれど
That makes sense, because the separable differential equations are really just implicit derivatives backwards.
xを満たす数値が複数存在し得ます 微分方程式は
If you have a polynomial, you could have more than one values of x that satisfy this equation.
関数です とにかく これは微分方程式の
The solution to a differential equation is not a number, it is a function.
微分は xとyのある関数に等しいです
And as we see right here, we have the derivative.
平均も相関係数も回帰係数も
And that's true of any sample statistic.
この微分は
Here we just use our implicit differentiation skills.
偏微分の項
Eventually, this capital delta
psi x y の微分が 0または定数Cとなる psi x y の微分が 0または定数Cとなる 答えが得られます
And if it's an exact equation, that tells us that there exists a psi, such that the derivative of psi of x, y is equal to 0, or psi of x, y is equal to c, is a solution of this equation.
相関係数
Correlation
消散係数
Extinction
冷却係数
Cooling factor
定数の1をxで微分しても 0になります
The derivative of X 2 is 2X, the derivative with respect to X of pi of a constant is just 0.
微分方程式は何次ですか 最高の導関数は
So first of all, what is the order of this differential equation?
微分方程式の力学で 最終的に 変数は120よ
In total, we are talking about 120 variables in a dynamic system of differential equations.
二階の導関数の定数の係数です Bは 一階の導関数の定数の係数で 定数Cがyの係数です
So I can just rewrite that as A so now A is not a function anymore, it's just a number A times the second derivative of y, with respect to x, plus B times the first derivative, plus C times y.
ここに負の記号がありますがこれは微分の チェーンルールを使う際対数の式の微分からです
The first derivative of this expression over here is number 7, and it's interesting it's not number 2.
偏微分ではなく 完全微分を取るには xに関する偏微分と yに関する偏微分にdy dxを掛けたものを
If psi is a function of x and y, and I would take not a partial derivative, I would take the full derivative of psi with respect to x, it's equal to the partial of psi with respect to x, plus the partial of psi with respect to y, times dy dx.
変数分離形微分方程式は 積分の一般解を逆に 行うものです
And I know we did a couple already, but another way to think about separable differential equations is really, all you're doing is implicit differentiation in reverse.
数学教師が偏微分の概念について説明した
The math teacher explained the concept of partial differentiation.
微分は 本当に
That's what a differential essentially is.
特に 微分クラスで
I expect you to see.
xとyの関数の psi のxに関する偏微分 これが0になります 微分方程式が この形で
You could rewrite, this is just the derivative of psi, with respect to x, inside the function of x, y, is equal to 0.
xに関するpsi の微分は psi は x とyの関数で 0です これは x に関して psi の微分です
So hopefully this gives you a little intuition of why we can just rewrite this equation as the derivative with respect x of psi, which is a function of x and y, is equal to 0.
一見不可分の微分を
And we're done.

 

関連検索 : 数学微積分 - 分配係数 - 部分係数 - 分配係数 - 分配係数 - 分割係数 - 分散係数 - 分配係数 - 分離係数 - 微系数 - 係数 - 係数 - 微分値 - 微積分