a)\(sin^2\left(180^o-\alpha\right)+tan^2\left(180-\alpha\right).tan^2\left(270^o+\alpha\right)\)\(+sin\left(90^o+\alpha\right)cos\left(\alpha-360^o\right)\)
\(=sin^2\alpha+tan^2\alpha.cot^2\alpha+cos\alpha cos\alpha\)
\(=sin^2\alpha+cos^2\alpha+\left(tan\alpha cot\alpha\right)^2=1+1=2\).

\(\dfrac{cos\left(\alpha-180^o\right)}{sin\left(180^o-\alpha\right)}+\dfrac{tan\left(\alpha-180^o\right)cos\left(180^o+\alpha\right)sin\left(270^o+\alpha\right)}{tan\left(270^o+\alpha\right)}\)
\(=\dfrac{cos\left(180^o-\alpha\right)}{sin\left(180^o-\alpha\right)}+\dfrac{-tan\left(180^o-\alpha\right).cos\alpha.sin\left(90^o+\alpha\right)}{-tan\left(90^o+\alpha\right)}\)
\(=tan\left(180^o-\alpha\right)+\dfrac{tan\alpha.cos\alpha.cos\alpha}{cot\alpha}\)
\(=-tan\alpha+tan^2\alpha cos^2\alpha\)
\(=tan\alpha\left(-1+tan\alpha cos^2\alpha\right)\)
\(=tan\alpha\left(sin\alpha cos\alpha-1\right)\).

c) \(\dfrac{cos\left(-288^o\right)cot72^o}{tan\left(-162^o\right)sin108^o}-tan18^o\)
\(=\dfrac{cos72^ocot72^o}{tan18^o.sin72^o}-tan18^o\)
\(=\dfrac{cos^272^o.cos18^o}{sin72^osin18^o.sin72^o}-tan18^o\)
\(=cot^272^ocot18^o-tan18^o\)
\(=tan^218^ocot18^o-tan18^o\)
\(=tan18^o-tan18^o=0\).

a) Ta có A=\dfrac{\tan \alpha+3 \dfrac{1}{\tan \alpha}}{\tan \alpha+\dfrac{1}{\tan \alpha}}=\dfrac{\tan ^{2} \alpha+3}{\tan ^{2} \alpha+1}=\dfrac{\dfrac{1}{\cos ^{2} \alpha}+2}{\dfrac{1}{\cos ^{2} \alpha}}=1+2 \cos ^{2} \alphaA=tanα+tanα1​tanα+3tanα1​​=tan2α+1tan2α+3​=cos2α1​cos2α1​+2​=1+2cos2α Suy ra A=1+2 \cdot \dfrac{9}{16}=\dfrac{17}{8}A=1+2⋅169​=817​.

b) B=\dfrac{\dfrac{\sin \alpha}{\cos ^{3} \alpha}-\dfrac{\cos \alpha}{\cos ^{3} \alpha}}{\dfrac{\sin ^{3} \alpha}{\cos ^{3} \alpha}+\dfrac{3 \cos ^{3} \alpha}{\cos ^{3} \alpha}+\dfrac{2 \sin \alpha}{\cos ^{3} \alpha}}=\dfrac{\tan \alpha\left(\tan ^{2} \alpha+1\right)-\left(\tan ^{2} \alpha+1\right)}{\tan ^{3} \alpha+3+2 \tan \alpha\left(\tan ^{2} \alpha+1\right)}B=cos3αsin3α​+cos3α3cos3α​+cos3α2sinα​cos3αsinα​−cos3αcosα​​=tan3α+3+2tanα(tan2α+1)tanα(tan2α+1)−(tan2α+1)​.

Suy ra B=\dfrac{\sqrt{2}(2+1)-(2+1)}{2 \sqrt{2}+3+2 \sqrt{2}(2+1)}=\dfrac{3(\sqrt{2}-1)}{3+8 \sqrt{2}}B=22​+3+22​(2+1)2​(2+1)−(2+1)​=3+82​3(2​−1)​.

b) \(\sin x+\cos x=\dfrac{3}{2}\)

\(\left(\sin x+\cos x\right)^2=\dfrac{1}{4}\)

\(\sin^2x+\cos^2x+2\sin x\cos x=\dfrac{1}{4}\)

\(2\sin x\cos x=-\dfrac{3}{4}=\sin2x\)

ý a,

ý c

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:

\(\begin{array}{l}\cot \alpha  = \frac{{\cos \alpha }}{{\sin \alpha }};\;\\ \Rightarrow \;1 + {\cot ^2}\alpha  = 1 + \frac{{{{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha  + {{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{1}{{{{\sin }^2}\alpha }}\;\end{array}\)

\(90^0< a< 180^0\)

=>\(cosa< 0\)

\(sin^2a+cos^2a=1\)

=>\(cos^2a=1-\left(\dfrac{1}{3}\right)^2=\dfrac{8}{9}\)

mà cosa<0

nên \(cosa=-\dfrac{2\sqrt{2}}{3}\)

\(tan\left(180^0-a\right)=-tana=-\dfrac{sina}{cosa}\)

\(=-\dfrac{1}{3}:\dfrac{-2\sqrt{2}}{3}=\dfrac{1}{2\sqrt{2}}=\dfrac{\sqrt{2}}{4}\)

Tham khảo:

a) 

Gọi M(x;y) là điểm trên đường tròn đơn vị sao cho \(\widehat {xOM} = \alpha \). Gọi N, P tương ứng là hình chiếu vuông góc của M lên các trục Ox, Oy.

Ta có: \(\left\{ \begin{array}{l}x = \cos \alpha \\y = \sin \alpha \end{array} \right. \Rightarrow \left\{ \begin{array}{l}{\cos ^2}\alpha  = {x^2}\\{\sin ^2}\alpha  = {y^2}\end{array} \right.\)(1)

Mà \(\left\{ \begin{array}{l}\left| x \right| = ON\\\left| y \right| = OP = MN\end{array} \right. \Rightarrow \left\{ \begin{array}{l}{x^2} = {\left| x \right|^2} = O{N^2}\\{y^2} = {\left| y \right|^2} = M{N^2}\end{array} \right.\)(2)

Từ (1) và (2) suy ra \({\sin ^2}\alpha  + {\cos ^2}\alpha  = O{N^2} + M{N^2} = O{M^2}\) (do \(\Delta OMN\) vuông tại N)

\( \Rightarrow {\sin ^2}\alpha  + {\cos ^2}\alpha  = 1\) (vì OM =1). (đpcm)

b) 

Ta có:  \(\tan \alpha  = \frac{{\sin \alpha }}{{\cos \alpha }}\;\;(\alpha  \ne {90^o})\)

\( \Rightarrow 1 + {\tan ^2}\alpha  = 1 + \frac{{{{\sin }^2}\alpha }}{{{{\cos }^2}\alpha }} = \frac{{{{\cos }^2}\alpha }}{{{{\cos }^2}\alpha }} + \frac{{{{\sin }^2}\alpha }}{{{{\cos }^2}\alpha }} = \frac{{{{\sin }^2}\alpha  + {{\cos }^2}\alpha }}{{{{\cos }^2}\alpha }}\)

Mà theo ý a) ta có \({\sin ^2}\alpha  + {\cos ^2}\alpha  = 1\) với mọi góc \(\alpha \)

\( \Rightarrow 1 + {\tan ^2}\alpha  = \frac{1}{{{{\cos }^2}\alpha }}\) (đpcm)

c) 

Ta có:  \(\cot \alpha  = \frac{{\cos \alpha }}{{\sin \alpha }}\;\;\;({0^o} < \alpha  < {180^o})\)

\( \Rightarrow 1 + {\cot ^2}\alpha  = 1 + \frac{{{{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha }}{{{{\sin }^2}\alpha }} + \frac{{{{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }} = \frac{{{{\sin }^2}\alpha  + {{\cos }^2}\alpha }}{{{{\sin }^2}\alpha }}\)

Mà theo ý a) ta có \({\sin ^2}\alpha  + {\cos ^2}\alpha  = 1\) với mọi góc \(\alpha \)

\( \Rightarrow 1 + {\cot ^2}\alpha  = \frac{1}{{{{\sin }^2}\alpha }}\) (đpcm)

\(P=\dfrac{2sin\alpha-3cos\alpha}{3sin\alpha+2cos\alpha}\\ =\dfrac{\dfrac{2sin\alpha}{cos\alpha}-\dfrac{3cos\alpha}{cos\alpha}}{\dfrac{3sin\alpha}{cos\alpha}+\dfrac{2cos\alpha}{cos\alpha}}\\ =\dfrac{2tan\alpha-3}{3tan\alpha+2}=\dfrac{2.3-3}{3.3+2}=\dfrac{3}{11}\)

Ta có: \(1 + {\tan ^2}\alpha  = \frac{1}{{{{\cos }^2}\alpha }}\quad (\alpha  \ne {90^o})\)

\( \Rightarrow \frac{1}{{{{\cos }^2}\alpha }} = 1 + {3^2} = 10\)

\( \Leftrightarrow {\cos ^2}\alpha  = \frac{1}{{10}} \Leftrightarrow \cos \alpha  =  \pm \frac{{\sqrt {10} }}{{10}}\)

Vì \({0^o} < \alpha  < {180^o}\) nên \(\sin \alpha  > 0\).

Mà \(\tan \alpha  = 3 > 0 \Rightarrow \cos \alpha  > 0 \Rightarrow \cos \alpha  = \frac{{\sqrt {10} }}{{10}}\)

Lại có: \(\sin \alpha  = \cos \alpha .\tan \alpha  = \frac{{\sqrt {10} }}{{10}}.3 = \frac{{3\sqrt {10} }}{{10}}.\)

\( \Rightarrow P = \dfrac{{2.\frac{{3\sqrt {10} }}{{10}} - 3.\frac{{\sqrt {10} }}{{10}}}}{{3.\frac{{3\sqrt {10} }}{{10}} + 2.\frac{{\sqrt {10} }}{{10}}}} = \dfrac{{\frac{{\sqrt {10} }}{{10}}\left( {2.3 - 3} \right)}}{{\frac{{\sqrt {10} }}{{10}}\left( {3.3 + 2} \right)}} = \dfrac{3}{{11}}.\)

\(0< a< 90^0\)

=>\(sina>0\)

\(sin^2a+cos^2a=1\)

=>\(sin^2a=1-\dfrac{9}{16}=\dfrac{7}{16}\)

=>\(sina=\dfrac{\sqrt{7}}{4}\)

\(tana=\dfrac{sina}{cosa}=\dfrac{\sqrt{7}}{4}:\dfrac{3}{4}=\dfrac{\sqrt{7}}{3}\)

\(cota=\dfrac{1}{tana}=\dfrac{3}{\sqrt{7}}\)

\(A=\dfrac{tana+3cota}{tana+cota}=\dfrac{\dfrac{\sqrt{7}}{3}+\dfrac{9}{\sqrt{7}}}{\dfrac{3}{\sqrt{7}}+\dfrac{\sqrt{7}}{3}}\)

\(=\dfrac{34}{3\sqrt{7}}:\dfrac{16}{3\sqrt{7}}=\dfrac{17}{8}\)