fix(ch7): correct convolution example sign, fix cos^2 transform
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@@ -130,7 +130,7 @@ The following table collects the most commonly used Laplace transforms. Each ent
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$e^{at}\sin(bt)$ & $\dfrac{b}{(s-a)^2 + b^2}$ & $s > a$ \\[10pt]
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$e^{at}\sin(bt)$ & $\dfrac{b}{(s-a)^2 + b^2}$ & $s > a$ \\[10pt]
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$e^{at}\cos(bt)$ & $\dfrac{s-a}{(s-a)^2 + b^2}$ & $s > a$ \\[10pt]
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$e^{at}\cos(bt)$ & $\dfrac{s-a}{(s-a)^2 + b^2}$ & $s > a$ \\[10pt]
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$\sin^2(bt)$ & $\dfrac{2b^2}{s(s^2 + 4b^2)}$ & $s > 0$ \\[10pt]
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$\sin^2(bt)$ & $\dfrac{2b^2}{s(s^2 + 4b^2)}$ & $s > 0$ \\[10pt]
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$\cos^2(bt)$ & $\dfrac{s^2}{(s^2 + 4b^2)(s)}$ & $s > 0$ \\[10pt]
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$\cos^2(bt)$ & $\dfrac{s^2+2b^2}{s(s^2 + 4b^2)}$ & $s > 0$ \\[10pt]
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$t\sin(bt)$ & $\dfrac{2bs}{(s^2 + b^2)^2}$ & $s > 0$ \\[10pt]
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$t\sin(bt)$ & $\dfrac{2bs}{(s^2 + b^2)^2}$ & $s > 0$ \\[10pt]
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$t\cos(bt)$ & $\dfrac{s^2 - b^2}{(s^2 + b^2)^2}$ & $s > 0$ \\[10pt]
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$t\cos(bt)$ & $\dfrac{s^2 - b^2}{(s^2 + b^2)^2}$ & $s > 0$ \\[10pt]
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$u_c(t)$ \quad (Heaviside step) & $\dfrac{e^{-cs}}{s}$ & $s > 0$ \\[10pt]
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$u_c(t)$ \quad (Heaviside step) & $\dfrac{e^{-cs}}{s}$ & $s > 0$ \\[10pt]
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@@ -843,15 +843,15 @@ The inner integral is $G(s)$, and the remaining integral is $F(s)$. Thus the res
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\[
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\[
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\begin{aligned}
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\begin{aligned}
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\int_0^t \tau\,\sin(t-\tau)\,\diff\tau
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\int_0^t \tau\,\sin(t-\tau)\,\diff\tau
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&= \Bigl[-\tau\cos(t-\tau)\Bigr]_0^t + \int_0^t \cos(t-\tau)\,\diff\tau \\
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&= \Bigl[\tau\cos(t-\tau)\Bigr]_0^t - \int_0^t \cos(t-\tau)\,\diff\tau \\
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&= \bigl(-t\cos(0) - 0\bigr) + \Bigl[-\sin(t-\tau)\Bigr]_0^t \\
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&= \bigl(t\cos(0) - 0\bigr) - \Bigl[-\sin(t-\tau)\Bigr]_0^t \\
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&= -t + \bigl(-\sin(0) + \sin(t)\bigr) \\
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&= t - \bigl(-\sin(0) + \sin(t)\bigr) \\
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&= \sin(t) - t.
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&= t - \sin(t).
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\end{aligned}
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\end{aligned}
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\]
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\]
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Therefore:
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Therefore:
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\[
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\[
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\mathcal{L}^{-1}\left\{\frac{1}{s^2(s^2+1)}\right\} = \sin(t) - t.
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\mathcal{L}^{-1}\left\{\frac{1}{s^2(s^2+1)}\right\} = t - \sin(t).
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\]
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\]
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\end{workedexample}
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\end{workedexample}
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