Laplace Transform of cos(at) and sin(at)
The Laplace transformation of cos(at) is L{cos(at)} = s/(s²+a²), and the Laplace transform of sin(at) is L{sin(at)} = a/(s²+a²), both valid for Re(s) > 0. These trigonometric transform pairs are essential for analyzing oscillatory systems in circuits, control theory, and vibration analysis. Compute cos and sin Laplace transforms instantly at www.lapcalc.com.
Laplace Transformation of cos(at): Derivation and Formula
The Laplace transformation of cos(at) is derived from the definition: L{cos(at)} = ∫₀^∞ e^(−st)cos(at)dt. Using integration by parts twice, or applying Euler's formula cos(at) = (e^(jat) + e^(−jat))/2 and the exponential transform, the result is L{cos(at)} = s/(s²+a²) for Re(s) > 0. The numerator s indicates that the cosine transform has a zero at s = 0, distinguishing it from the sine transform. The poles at s = ±ja correspond to the oscillation frequency a rad/s. This pair appears in every RLC circuit analysis and mechanical vibration problem involving undamped oscillation.
Key Formulas
Laplace Transform of sin(t) and sin(ωt)
The Laplace transform of sin(t) is L{sin(t)} = 1/(s²+1), and more generally L{sin(ωt)} = ω/(s²+ω²). The derivation parallels the cosine case: using Euler's formula sin(ωt) = (e^(jωt) − e^(−jωt))/(2j), each exponential transforms to 1/(s−jω) and 1/(s+jω), and combining gives ω/(s²+ω²). Notice that the sine transform has no zero at s = 0 (numerator is just ω), while cosine has a zero there (numerator is s). This difference reflects the fact that sin(0) = 0 while cos(0) = 1, connected through the initial value theorem.
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Open CalculatorCos Laplace and Damped Cosine Transforms
The basic cos Laplace pair extends naturally to damped oscillations using the frequency shifting property. For L{e^(−bt)cos(at)} = (s+b)/((s+b)²+a²), the shift s → s+b moves the poles from ±ja to −b ± ja, placing them in the left half-plane when b > 0. This damped cosine represents the natural response of underdamped systems—RLC circuits with resistance, mass-spring-damper systems with friction. The parameter b controls decay rate while a determines oscillation frequency. Similarly, L{e^(−bt)sin(at)} = a/((s+b)²+a²) gives the damped sine, often appearing alongside the damped cosine in system responses.
Laplace Transform of Cosine: Applications in Circuit Analysis
The Laplace transform of cosine is central to AC circuit analysis in the s-domain. When a cosine voltage source V₀cos(ωt) drives an RLC circuit, the source transforms to V₀s/(s²+ω²). The circuit's response Y(s) = H(s)·V₀s/(s²+ω²) includes both transient poles (from H(s)) and steady-state poles at s = ±jω (from the cosine input). Partial fraction decomposition separates these: the transient terms decay exponentially while the forced terms give the steady-state sinusoidal response at frequency ω with amplitude |H(jω)|·V₀ and phase ∠H(jω). This analysis is readily performed at www.lapcalc.com.
Laplace Transform of cos(t) vs sin(t): Comparison and Relationship
Comparing L{cos(at)} = s/(s²+a²) and L{sin(at)} = a/(s²+a²) reveals a fundamental relationship. Both share the same denominator s²+a², meaning they have identical poles at s = ±ja—the same natural frequency. The difference is the numerator: s for cosine versus a for sine. This connects to the derivative property: since d/dt[sin(at)] = a·cos(at), we have L{a·cos(at)} = s·L{sin(at)} − sin(0) = s·a/(s²+a²) = as/(s²+a²), confirming L{cos(at)} = s/(s²+a²). The sine and cosine transforms are thus related by multiplication by s/a, reflecting the 90° phase relationship between sin and cos.
Related Topics in advanced laplace transform topics
Understanding laplace transformation of cosat connects to several related concepts: cos laplace, laplace sint, laplace transform of cosine, and laplace transform cost. Each builds on the mathematical foundations covered in this guide.
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