Resposta: [tex]\displaystyle\int_{-\pi/\omega}^{\pi/\omega}t\,\mathrm{sen}(k\omega t)\,dt=\left\{\begin{array}{ll}0~\mathrm{(zero)},&\mathrm{se~}k=0\\\\ (-1)^{k+1}\cdot \dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\ne 0\end{array}\right..[/tex]
Explicação passo a passo:
Calcular a integral definida:
[tex]\displaystyle\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(k\omega t)\,dt[/tex]
com k inteiro e ω ≠ 0.
[tex]=\displaystyle\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(0\cdot \omega t)\,dt\\\\\\=\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(0)\,dt\\\\\\=\int_{-\pi/\omega}^{\pi/\omega} 0\,dt=0.[/tex]
[tex]\begin{array}{lcl}u=t&\quad\Longrightarrow\quad&du=dt\\\\dv=\mathrm{sen}(k\omega t)\,dt&\quad\Longleftarrow\quad&v=-\,\dfrac{1}{k\omega}\cos(k\omega t)\end{array}[/tex]
[tex]\displaystyle\int_a^b u\,dv=uv\Big|_a^b-\int_a^b v\,du[/tex]
[tex]\begin{array}{lcr}\displaystyle\Longrightarrow \quad\int_{-\pi/\omega}^{\pi/\omega}t\,\mathrm{sen}(k\omega t)\,dt&\!\!=\!\!& t\cdot \left[-\,\dfrac{1}{k\omega}\cos(k\omega t)\right]_{-\pi/\omega}^{\pi/\omega}\\\\&&\displaystyle -\int_{-\pi/\omega}^{\pi/\omega}\left[-\,\frac{1}{k\omega}\cos(k\omega t)\right]\!dt\end{array}[/tex]
[tex]\displaystyle=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\frac{1}{k\omega}\int_{-\pi/\omega}^{\pi/\omega}\cos(k\omega t)\,dt\\\\\\=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\frac{1}{k\omega}\cdot \left.\frac{1}{k\omega}\,\mathrm{sen}(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}[/tex]
[tex]\displaystyle=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\left.\frac{1}{(k\omega)^2}\,\mathrm{sen}(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}[/tex]
[tex]\begin{array}{lr}=\!\!\!&\left[-\dfrac{~\frac{\pi}{\omega}~}{k\omega}\cos\!\left(k\omega\cdot \dfrac{\pi}{\omega}\right)+\dfrac{~-\frac{\pi}{\omega}~}{k\omega}\cos\!\left(k\omega \cdot -\dfrac{\pi}{\omega}\right)\right]\\\\&+\left[\dfrac{1}{(k\omega)^2}\,\mathrm{sen}\!\left(k\omega\cdot \dfrac{\pi}{\omega}\right)-\dfrac{1}{(k\omega)^2}\,\mathrm{sen}\!\left(k\omega\cdot -\dfrac{\pi}{\omega}\right)\right]\end{array}[/tex]
[tex]=\left[-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)\right]+\underbrace{\left[\dfrac{1}{(k\omega)^2}\,\mathrm{sen}(k\pi)-\dfrac{1}{(k\omega)^2}\,\mathrm{sen}(-k\pi)\right]}_{=0\mathrm{~(zero),~pois}~sen(\pm\,k\pi)=0}[/tex]
[tex]=\left[-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)\right]+0\\\\\\=-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)[/tex]
Como o cosseno é uma função par, temos cos(− kπ) = cos(kπ). Então, o resultado fica
[tex]=-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(k\pi)\\\\\\=-\,\dfrac{2\pi}{k\omega^2}\cos(k\pi)[/tex]
[tex]=\left\{\begin{array}{ll}-\,\dfrac{2\pi}{k\omega^2}\cdot 1,&\mathrm{se~}k\mathrm{~for~par}\\\\-\,\dfrac{2\pi}{k\omega^2}\cdot (-1),&\mathrm{se~}k\mathrm{~for~\'impar}\end{array}\right.[/tex]
[tex]=\left\{\begin{array}{rl}-\,\dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\mathrm{~for~par}\\\\\dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\mathrm{~for~\'impar}\end{array}\right.[/tex]
[tex]=(-1)^{k+1}\cdot \dfrac{2\pi}{k\omega^2}\quad\longleftarrow\quad \mathsf{resposta~para~}k\ne 0.[/tex]
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Resposta: [tex]\displaystyle\int_{-\pi/\omega}^{\pi/\omega}t\,\mathrm{sen}(k\omega t)\,dt=\left\{\begin{array}{ll}0~\mathrm{(zero)},&\mathrm{se~}k=0\\\\ (-1)^{k+1}\cdot \dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\ne 0\end{array}\right..[/tex]
Explicação passo a passo:
Calcular a integral definida:
[tex]\displaystyle\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(k\omega t)\,dt[/tex]
com k inteiro e ω ≠ 0.
[tex]=\displaystyle\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(0\cdot \omega t)\,dt\\\\\\=\int_{-\pi/\omega}^{\pi/\omega} t\,\mathrm{sen}(0)\,dt\\\\\\=\int_{-\pi/\omega}^{\pi/\omega} 0\,dt=0.[/tex]
[tex]\begin{array}{lcl}u=t&\quad\Longrightarrow\quad&du=dt\\\\dv=\mathrm{sen}(k\omega t)\,dt&\quad\Longleftarrow\quad&v=-\,\dfrac{1}{k\omega}\cos(k\omega t)\end{array}[/tex]
[tex]\displaystyle\int_a^b u\,dv=uv\Big|_a^b-\int_a^b v\,du[/tex]
[tex]\begin{array}{lcr}\displaystyle\Longrightarrow \quad\int_{-\pi/\omega}^{\pi/\omega}t\,\mathrm{sen}(k\omega t)\,dt&\!\!=\!\!& t\cdot \left[-\,\dfrac{1}{k\omega}\cos(k\omega t)\right]_{-\pi/\omega}^{\pi/\omega}\\\\&&\displaystyle -\int_{-\pi/\omega}^{\pi/\omega}\left[-\,\frac{1}{k\omega}\cos(k\omega t)\right]\!dt\end{array}[/tex]
[tex]\displaystyle=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\frac{1}{k\omega}\int_{-\pi/\omega}^{\pi/\omega}\cos(k\omega t)\,dt\\\\\\=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\frac{1}{k\omega}\cdot \left.\frac{1}{k\omega}\,\mathrm{sen}(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}[/tex]
[tex]\displaystyle=\left.-\,\frac{t}{k\omega}\cos(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}+\left.\frac{1}{(k\omega)^2}\,\mathrm{sen}(k\omega t)\right|_{-\pi/\omega}^{\pi/\omega}[/tex]
[tex]\begin{array}{lr}=\!\!\!&\left[-\dfrac{~\frac{\pi}{\omega}~}{k\omega}\cos\!\left(k\omega\cdot \dfrac{\pi}{\omega}\right)+\dfrac{~-\frac{\pi}{\omega}~}{k\omega}\cos\!\left(k\omega \cdot -\dfrac{\pi}{\omega}\right)\right]\\\\&+\left[\dfrac{1}{(k\omega)^2}\,\mathrm{sen}\!\left(k\omega\cdot \dfrac{\pi}{\omega}\right)-\dfrac{1}{(k\omega)^2}\,\mathrm{sen}\!\left(k\omega\cdot -\dfrac{\pi}{\omega}\right)\right]\end{array}[/tex]
[tex]=\left[-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)\right]+\underbrace{\left[\dfrac{1}{(k\omega)^2}\,\mathrm{sen}(k\pi)-\dfrac{1}{(k\omega)^2}\,\mathrm{sen}(-k\pi)\right]}_{=0\mathrm{~(zero),~pois}~sen(\pm\,k\pi)=0}[/tex]
[tex]=\left[-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)\right]+0\\\\\\=-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(-k\pi)[/tex]
Como o cosseno é uma função par, temos cos(− kπ) = cos(kπ). Então, o resultado fica
[tex]=-\dfrac{\pi}{k\omega^2}\cos(k\pi)-\dfrac{\pi}{k\omega^2}\cos(k\pi)\\\\\\=-\,\dfrac{2\pi}{k\omega^2}\cos(k\pi)[/tex]
[tex]=\left\{\begin{array}{ll}-\,\dfrac{2\pi}{k\omega^2}\cdot 1,&\mathrm{se~}k\mathrm{~for~par}\\\\-\,\dfrac{2\pi}{k\omega^2}\cdot (-1),&\mathrm{se~}k\mathrm{~for~\'impar}\end{array}\right.[/tex]
[tex]=\left\{\begin{array}{rl}-\,\dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\mathrm{~for~par}\\\\\dfrac{2\pi}{k\omega^2},&\mathrm{se~}k\mathrm{~for~\'impar}\end{array}\right.[/tex]
[tex]=(-1)^{k+1}\cdot \dfrac{2\pi}{k\omega^2}\quad\longleftarrow\quad \mathsf{resposta~para~}k\ne 0.[/tex]
Dúvidas? Comente.
Bons estudos.