Correct Answer - Option 1 :
\(\frac{\omega }{{{{\left( {s + a} \right)}^2} + {\omega ^2}}}\)
Concept:
Bilateral Laplace transform:
\(L\left[ {x\left( t \right)} \right] = x\left( s \right) = \;\mathop \smallint \limits_{ - \infty }^\infty x\left( t \right){e^{ - st}}dt\)
Unilateral Laplace transform:
\(L\left[ {x\left( t \right)} \right] = x\left( s \right) = \;\mathop \smallint \limits_0^\infty x\left( t \right){e^{ - st}}dt\)
Some important Laplace transforms:
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f(t)
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f(s)
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ROC
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1.
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δ(t)
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1
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Entire s-plane
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2.
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e-at u(t)
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\(\frac{1}{{s + a}}\)
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s > - a
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3.
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e-at u(-t)
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\(\frac{1}{{s + a}}\)
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s < - a
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4.
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cos ω0 t u(t)
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\(\frac{s}{{{s^2} + \omega _0^2}}\)
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s > 0
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5.
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te-at u(t)
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\(\frac{1}{{{{\left( {s + a} \right)}^2}}}\)
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s > - a
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6.
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sin ω0t u(t)
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\(\frac{{{\omega _0}}}{{{s^2} + \omega _0^2}}\)
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s > 0
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7.
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u(t)
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1/s
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s > 0
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Calculation:
\(\sin \omega t. u(t)\leftrightarrow \frac{\omega }{{{s^2} + {\omega ^2}}}\)
By applying frequency differentiation property,
\({e^{ - at}}\sin \omega t. u(t) \leftrightarrow \frac{\omega }{{{{\left( {s + a} \right)}^2} + {\omega ^2}}}\)