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JEE Main 202329 JanuaryEvening Shift
Exam
JEE Main
Year
2023
Date
29 January
Shift
Evening Shift
Subject
Mathematics
Chapter
Matrices

JEE Main 2023 · 29 January · Evening Shift · Mathematics · Matrices

The set of all values of t ∈ ℝ , for which the matrix [ cases e ^ t...

The set of all values of t∈Rt \in \mathbb{R}, for which the matrix \left[{ete−t(sin⁡t−2cos⁡t)e−t(−2sin⁡t−cos⁡t)ete−t(2sin⁡t+cos⁡t)e−t(sin⁡t−2cos⁡t)ete−tcos⁡te−tsin⁡t\begin{cases}{e}^{t} & {e}^{- t}\left(\sin t - 2\cos t\right) & {e}^{- t}\left(- 2\sin t - \cos t\right) \\ {e}^{t} & {e}^{- t}\left(2\sin t + \cos t\right) & {e}^{- t}\left(\sin t - 2\cos t\right) \\ {e}^{t} & {e}^{- t}\cos t & {e}^{- t}\sin t\end{cases}\right] is invertible, is

Options

  1. A{(2k+1)π2,k∈Z}\left\{\left(2k + 1\right)\dfrac{\pi}{2}, k \in \mathbb{Z}\right\}
  2. B{kπ+π4,k∈Z}\left\{k\pi + \dfrac{\pi}{4}, k \in \mathbb{Z}\right\}
  3. C{kπ,k∈Z}\left\{k\pi, k \in \mathbb{Z}\right\}
  4. DR\mathbb{R}

Correct answer

D. R\mathbb{R}

Step-by-step solution

Let

A = \left[\begin{cases}{e}^{t} & {e}^{- t}\left(\sin t - 2\cos t\right) & {e}^{- t}\left(- 2\sin t - \cos t\right) \\ {e}^{t} & {e}^{- t}\left(2\sin t + \cos t\right) & {e}^{- t}\left(\sin t - 2\cos t\right) \\ {e}^{t} & {e}^{- t}\cos t & {e}^{- t}\sin t\end{cases}\right]

Given matrix AA is invertible if

\left|A\right| \ne 0</p><p></p><p>⇒ \left|ete−t(sin⁡t−2cos⁡t)e−t(−2sin⁡t−cos⁡t)ete−t(2sin⁡t+cos⁡t)e−t(sin⁡t−2cos⁡t)ete−tcos⁡te−tsin⁡t\begin{array}{ll}{e}^{t} {e}^{- t}\left(\sin t - 2\cos t\right) {e}^{- t}\left(- 2\sin t - \cos t\right) \\ {e}^{t} & {e}^{- t}\left(2\sin t + \cos t\right) & {e}^{- t}\left(\sin t - 2\cos t\right) \\ {e}^{t} & {e}^{- t}\cos t & {e}^{- t}\sin t\end{array}\right| \ne 0</p><p></p><p>⇒ {e}^{t} \cdot {e}^{- t} \cdot {e}^{- t}\left|{1sin⁡t−2cos⁡t−2sin⁡t−cos⁡t12sin⁡t+cos⁡tsin⁡t−2cos⁡t1cos⁡tsin⁡t\begin{cases}1 & \sin t - 2\cos t & - 2\sin t - \cos t \\ 1 & 2\sin t + \cos t & \sin t - 2\cos t \\ 1 & \cos t & \sin t\end{cases}\right| \ne 0</p><p>Applying</p><p>Applying{R}_{1} \to {R}_{1} - {R}_{2} then R2→R2−R3{R}_{2} \to {R}_{2} - {R}_{3}, ee get

{e}^{- t}\left|\begin{cases}0 & - \sin t - 3\cos t & - 3\sin t + \cos t \\ 0 & 2\sin t & - 2\cos t \\ 1 & \cos t & \sin t\end{cases}\right| \ne 0

By expanding we have,

e−t×(2sin⁡tcos⁡t+6cos⁡2t+6sin⁡2t−2sin⁡tcos⁡t)≠0{e}^{- t} \times \left(2\sin t \cos t + 6\cos^{2}t + 6\sin^{2}t - 2\sin t \cos t\right) \ne 0

⇒e−t×6≠0⇒ {e}^{- t} \times 6 \ne 0 for ∀t∈R\forall t \in \mathbb{R}

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