千秋岁·水边沙外
秦观
水边沙外。城郭春寒退。花影乱,莺声碎。飘零疏酒盏,离别宽衣带。人不见,碧云暮合空相对。
忆昔西池会。鹓鹭同飞盖。携手处,今谁在。日边清梦断,镜里朱颜改。春去也,飞红万点愁如海。
秦观
水边沙外。城郭春寒退。花影乱,莺声碎。飘零疏酒盏,离别宽衣带。人不见,碧云暮合空相对。
忆昔西池会。鹓鹭同飞盖。携手处,今谁在。日边清梦断,镜里朱颜改。春去也,飞红万点愁如海。
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In this section we explore the strong dependence of frequency response on the location of poles and zeros of \(H(s)\). This dependence points to a simple intuitive procedure to filter design.
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In this article, we show that a real signal \(x(t)\) whose spectrum is bandlimited to \(B\) Hz, i.e., \(X(\omega)=0\) for \(|\omega|>2 \pi B)\), can be reconstructed exactly (without any error) from its samples taken uniformly at a rate \(f_s>2 B\) samples per second. In other words, the minimum sampling frequency is \[ f_s>2 B \] Hz.
NOTE: In some literature, \(f_s=2 B\) is be used, which is not correct.
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The time-differentiation property of the Laplace transform has set the stage for solving linear differential (or integro-differential) equations with constant coefficients.
Because \(d^k y / d t^k \Longleftrightarrow\) \(s^k Y(s)\), the Laplace transform of a differential equation is an algebraic equation that can be readily solved for \(Y(s)\).
Next we take the inverse Laplace transform of \(Y(s)\) to find the desired solution \(y(t)\).
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For a quick reference table, see Wikipedia page on the Laplace transform.