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\(y'=\left(cosx\right)'\\ =\left(\dfrac{\pi}{2}-x\right)'cos\left(\dfrac{\pi}{2}-x\right)\\ =-cos\left(\dfrac{\pi}{2}-x\right)\\ =-sinx\)
\(f'\left(x0\right)=\lim\limits_{x\rightarrow x0}\dfrac{f\left(x\right)-f\left(x_0\right)}{x-x_0}\)
\(=\lim\limits_{x\rightarrow x0}\dfrac{sinx-sin\left(x0\right)}{x-x0}\)
\(=\lim\limits_{x\rightarrow x0}\dfrac{2\cdot cos\left(\dfrac{x+x0}{2}\right)\cdot sin\left(\dfrac{x-x0}{2}\right)}{x-x_0}\)
\(=\lim\limits_{x\rightarrow x0}\dfrac{2\cdot sin\left(\dfrac{x-x_0}{2}\right)\cdot cos\left(\dfrac{x+x_0}{2}\right)}{x-x_0}\)
\(=\lim\limits_{x\rightarrow x0}\dfrac{cos\left(x+x_0\right)}{2}=cos\left(x0\right)\)
=>\(\left(sinx'\right)=cosx\)
a: \(y=u^2=\left(sinx\right)^2\)
b: \(y'\left(x\right)=\left(sin^2x\right)'=2\cdot sinx\cdot cosx\)
\(y'\left(u\right)=\left(u^2\right)'=2\cdot u\)
\(u'\left(x\right)=\left(sinx\right)'=cosx\)
=>\(y'\left(x\right)=y'\left(u\right)\cdot u'\left(x\right)\)
tham khảo:
a)\(y'=xsin2x+sin^2x\)
\(y'=sin^2x+xsin2x\)
b)\(y'=-2sin2x+2cosx\\ y'=2\left(cosx-sin2x\right)\)
c)\(y=sin3x-3sinx\)
\(y'=3cos3x-3cosx\)
d)\(y'=\dfrac{1}{cos^2x}-\dfrac{1}{sin^2x}\)
\(y'=\dfrac{sin^2x-cos^2x}{sin^2x.cos^2x}\)
a) \(g'\left( x \right) = y' = {\left( {2x + \frac{\pi }{4}} \right)^,}.\cos \left( {2x + \frac{\pi }{4}} \right) = 2\cos \left( {2x + \frac{\pi }{4}} \right)\)
b) \(g'\left( x \right) = - 2{\left( {2x + \frac{\pi }{4}} \right)^,}.\sin \left( {2x + \frac{\pi }{4}} \right) = - 4\sin \left( {2x + \frac{\pi }{4}} \right)\)
\(a,y'=\left(f\left(g\left(x\right)\right)\right)'\)
\(=f'\left(g\left(x\right)\right).g'\left(x\right)\)
\(=e^{g\left(x\right)}.\left(2x-1\right)\)
\(=e^{x^2-x}.\left(2x-1\right)\)
\(b,y'=\dfrac{d}{dx}\left(3^{sinx}\right)\)
\(=\dfrac{d}{dx}\left(e^{ln3.sinx}\right)\)
\(=\dfrac{d}{dx}\left(ln3.sinx\right).e^{ln3.sinx}\)
\(=ln3.cosx.3^{sinx}\)
Với bất kì \({x_0} \in \mathbb{R}\), ta có:
\(f'\left( {{x_0}} \right) = \mathop {\lim }\limits_{x \to {x_0}} \frac{{f\left( x \right) - f\left( {{x_0}} \right)}}{{x - {x_0}}} = \mathop {\lim }\limits_{x \to {x_0}} \frac{{\sin x - \sin {x_0}}}{{x - {x_0}}}\)
Đặt \(x = {x_0} + \Delta x\). Ta có:
\(\begin{array}{l}f'\left( {{x_0}} \right) = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin \left( {{x_0} + \Delta x} \right) - \sin {x_0}}}{{\Delta x}} = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\cos \Delta x + \cos {x_0}\sin \Delta x - \sin {x_0}}}{{\Delta x}}\\ = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\cos \Delta x - \sin {x_0}}}{{\Delta x}} + \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\cos {x_0}\sin \Delta x}}{{\Delta x}} = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\left( {\cos \Delta x - 1} \right)}}{{\Delta x}} + \mathop {\lim }\limits_{\Delta x \to 0} \cos {x_0}.\mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin \Delta x}}{{\Delta x}}\end{array}\)
Lại có:
\(\begin{array}{l}\mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\left( {\cos \Delta x - 1} \right)}}{{\Delta x}} = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\left( {\cos \Delta x - 1} \right)\left( {\cos \Delta x + 1} \right)}}{{\Delta x\left( {\cos \Delta x + 1} \right)}} = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\left( {{{\cos }^2}\Delta x - 1} \right)}}{{\Delta x\left( {\cos \Delta x + 1} \right)}}\\ = \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}\left( { - {{\sin }^2}\Delta x} \right)}}{{\Delta x\left( {\cos \Delta x + 1} \right)}} = - \mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin \Delta x}}{{\Delta x}}.\mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin {x_0}.\sin \Delta x}}{{\left( {\cos \Delta x + 1} \right)}} = - 1.\frac{{\sin {x_0}.\sin 0}}{{\cos 0 + 1}} = 0\\\mathop {\lim }\limits_{\Delta x \to 0} \cos {x_0}.\mathop {\lim }\limits_{\Delta x \to 0} \frac{{\sin \Delta x}}{{\Delta x}} = \cos {x_0}.1 = \cos {x_0}\end{array}\)
Vậy \(f'\left( {{x_0}} \right) = \cos {x_0}\)
Vậy \(f'\left( x \right) = \cos x\) trên \(\mathbb{R}\).