Cho \(\tan\alpha=-2\sqrt{2}\) với \(0^0< \alpha< 90^0\). Tính \(\sin\alpha\) và \(\cos\alpha\) ?
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a) \({\cos ^2}\alpha + {\sin ^2}\alpha = 1\)
b) \(\tan \alpha .\cot \alpha = \frac{{\sin \alpha }}{{\cos \alpha }}.\frac{{\cos \alpha }}{{\sin \alpha }} = 1\)
c) \(\frac{{{{\sin }^2}\alpha + {{\cos }^2}\alpha }}{{{{\cos }^2}\alpha }} = \frac{{{{\sin }^2}\alpha }}{{{{\cos }^2}\alpha }} + \frac{{{{\cos }^2}\alpha }}{{{{\cos }^2}\alpha }} = {\tan ^2}\alpha + 1\)
d) \(\frac{1}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha + {{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha }}{{{{\sin }^2}\alpha }} + \frac{{{{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = 1 + {\cot ^2}\alpha \)
a)\(sin^2\left(180^o-\alpha\right)+tan^2\left(180-\alpha\right).tan^2\left(270^o+\alpha\right)\)\(+sin\left(90^o+\alpha\right)cos\left(\alpha-360^o\right)\)
\(=sin^2\alpha+tan^2\alpha.cot^2\alpha+cos\alpha cos\alpha\)
\(=sin^2\alpha+cos^2\alpha+\left(tan\alpha cot\alpha\right)^2=1+1=2\).
\(\dfrac{cos\left(\alpha-180^o\right)}{sin\left(180^o-\alpha\right)}+\dfrac{tan\left(\alpha-180^o\right)cos\left(180^o+\alpha\right)sin\left(270^o+\alpha\right)}{tan\left(270^o+\alpha\right)}\)
\(=\dfrac{cos\left(180^o-\alpha\right)}{sin\left(180^o-\alpha\right)}+\dfrac{-tan\left(180^o-\alpha\right).cos\alpha.sin\left(90^o+\alpha\right)}{-tan\left(90^o+\alpha\right)}\)
\(=tan\left(180^o-\alpha\right)+\dfrac{tan\alpha.cos\alpha.cos\alpha}{cot\alpha}\)
\(=-tan\alpha+tan^2\alpha cos^2\alpha\)
\(=tan\alpha\left(-1+tan\alpha cos^2\alpha\right)\)
\(=tan\alpha\left(sin\alpha cos\alpha-1\right)\).
\(tana-5cota+4=0\Rightarrow tana-\dfrac{5}{tana}+4=0\)
\(\Rightarrow tan^2a+4tana-5=0\Rightarrow\left[{}\begin{matrix}tana=1\\tana=-5\end{matrix}\right.\)
\(A=\dfrac{4sina+2cosa}{3sina-cosa}=\dfrac{\dfrac{4sina}{cosa}+\dfrac{2cosa}{cosa}}{\dfrac{3sina}{cosa}-\dfrac{cosa}{cosa}}=\dfrac{4tana+2}{3tana-1}=\left[{}\begin{matrix}3\\\dfrac{9}{8}\end{matrix}\right.\)
a)
Trên nửa đường tròn đơn vị, lấy điểm M sao cho \(\widehat {xOM} = \alpha \)
Gọi H, K lần lượt là các hình chiếu vuông góc của M trên Ox, Oy.
Ta có: tam giác vuông OHM vuông tại H và \(\alpha = \widehat {xOM}\)
Do đó: \(\sin \alpha = \frac{{MH}}{{OM}} = MH;\;\cos \alpha = \frac{{OH}}{{OM}} = OH.\)
\( \Rightarrow {\cos ^2}\alpha + {\sin ^2}\alpha = O{H^2} + M{H^2} = O{M^2} = 1\)
b) Ta có:
\(\begin{array}{l}\;\tan \alpha = \frac{{\sin \alpha }}{{\cos \alpha }};\;\cot \alpha = \frac{{\cos \alpha }}{{\sin \alpha }}.\\ \Rightarrow \;\tan \alpha .\cot \alpha = \frac{{\sin \alpha }}{{\cos \alpha }}.\frac{{\cos \alpha }}{{\sin \alpha }} = 1\end{array}\)
c) Với \(\alpha \ne {90^o}\) ta có:
\(\begin{array}{l}\;\tan \alpha = \frac{{\sin \alpha }}{{\cos \alpha }};\;\\ \Rightarrow \;1 + {\tan ^2}\alpha = 1 + \frac{{{{\sin }^2}\alpha }}{{{{\cos }^2}\alpha }} = \frac{{{{\sin }^2}\alpha + {{\cos }^2}\alpha }}{{{{\cos }^2}\alpha }} = \frac{1}{{{{\cos }^2}\alpha }}\;\end{array}\)
d) Ta có:
\(\begin{array}{l}\cot \alpha = \frac{{\cos \alpha }}{{\sin \alpha }};\;\\ \Rightarrow \;1 + {\cot ^2}\alpha = 1 + \frac{{{{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha + {{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{1}{{{{\sin }^2}\alpha }}\;\end{array}\)
b) \(\sin x+\cos x=\dfrac{3}{2}\)
\(\left(\sin x+\cos x\right)^2=\dfrac{1}{4}\)
\(\sin^2x+\cos^2x+2\sin x\cos x=\dfrac{1}{4}\)
\(2\sin x\cos x=-\dfrac{3}{4}=\sin2x\)
\(\sin\alpha=\dfrac{2\sqrt{2}}{3};\cos\alpha=\dfrac{1}{3}\)