Physics, asked by nikki6621, 3 months ago

Plzzz solve the problem​

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Answers

Answered by BrainlyEmpire
1

Given :-

 \rm \dfrac{tan A-Sin A }{tan A + Sin A } =  \dfrac{Sec A-1}{Sec A + 1}

To prove :

LHS = RHS

Proof :-

\rm RHS =  \dfrac{Sec A-1}{Sec A + 1}

\rm \:LHS =    \dfrac{tan A-Sin A }{tan A + Sin A }

 \rm  \rightarrow\dfrac{tan A-Sin A }{tan A + Sin A }

 \rm  \rightarrow\dfrac{ \dfrac{Sin  \: A}{cos \: A} -\dfrac{Sin  \: A}{ 1} }{ \dfrac{Sin  \: A}{cos \: A}  + \dfrac{Sin  \: A}{ 1}}  \\  \\ \rm  \rightarrow \:  \dfrac{Sin  \: A}{Sin  \: A}  \times  \bigg(\dfrac{ \dfrac{1}{cos \: A} -1 }{ \dfrac{1}{cos \: A}  +1}\bigg ) \\  \\ \rm  \rightarrow \:  1 \times \dfrac{ secA -1 }{  secA +1}\\  \\ \rm  \rightarrow \:  \dfrac{ secA -1 }{  secA +1}

Therefore, LHS = RHS

• hence proved!

Additional Information :-

\boxed{\begin{minipage}{6cm} Important Trigonometric identities :- \\ \\ $\: \: 1)\:\sin^2\theta+\cos^2\theta=1 \\ \\ 2)\:\sin^2\theta= 1-\cos^2\theta \\ \\ 3)\:\cos^2\theta=1-\sin^2\theta \\ \\ 4)\:1+\cot^2\theta=\text{cosec}^2 \, \theta \\ \\5)\: \text{cosec}^2 \, \theta-\cot^2\theta =1 \\ \\ 6)\:\text{cosec}^2 \, \theta= 1+\cot^2\theta \\\ \\ 7)\:\sec^2\theta=1+\tan^2\theta \\ \\ 8)\:\sec^2\theta-\tan^2\theta=1 \\ \\ 9)\:\tan^2\theta=\sec^2\theta-1$\end{minipage}}

Answered by Anonymous
7

Proper question :

Prove that :

\sf \dfrac {tanA \ - \ SinA}{tanA \ + \ SinA} \ = \ \dfrac {SecA \ - \ 1}{SecA \ + \ 1}

Given :

\sf \dfrac {tanA \ - \ SinA}{tanA \ + \ SinA} \ = \ \dfrac {SecA \ - \ 1}{SecA \ + \ 1}

To prove :

LHS = RHS

Proof :

\quad \sf LHS \ = \ \dfrac {tanA \ - \ SinA}{tanA \ + \ SinA}

\quad \sf RHS \ = \ \dfrac {SecA \ - \ 1}{SecA \ + \ 1}

\longrightarrow \sf \dfrac {tanA \ - \ SinA}{tanA \ + \ SinA}

\longrightarrow \sf \dfrac {\dfrac {sinA}{cosA} \ - \ \dfrac {SinA}{1}}{\dfrac {SinA}{cosA} \ + \ \dfrac {SinA}{1}}

\longrightarrow \sf \dfrac {SinA}{SinA} \times \bigg( \dfrac {\dfrac {1}{cosA} \ - \ 1}{\dfrac {1}{cosA} \ + \ 1 } \bigg)

\longrightarrow \sf 1 \times \dfrac {secA \ - \ 1}{secA \ + \ 1}

\longrightarrow \sf \dfrac {secA \ - \ 1}{secA \ + \ 1}

\sf = \ RHS

\therefore \large \sf LHS \ = \ RHS

Hence proved ✔︎

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