Active forum topics
- Problems in progression
- Ceva’s Theorem Is More Than a Formula for Concurrency
- The Chain Rule Explained: Don't Just Memorize, Visualize It
- The Intuition Behind Integration by Parts (Proof & Example)
- Statics
- Calculus
- Hydraulics: Rotating Vessel
- Inverse Trigo
- Hydraulics: Water is flowing through a pipe
- Application of Differential Equation: Newton's Law of Cooling
New forum topics
- Ceva’s Theorem Is More Than a Formula for Concurrency
- The Chain Rule Explained: Don't Just Memorize, Visualize It
- The Intuition Behind Integration by Parts (Proof & Example)
- Statics
- Calculus
- Hydraulics: Rotating Vessel
- Hydraulics: Water is flowing through a pipe
- Inverse Trigo
- Problems in progression
- General Solution of $y' = x \, \ln x$
Recent comments
- thankyouu!1 week 1 day ago
- z2 weeks 2 days ago
- Force P only impends motion…2 weeks 2 days ago
- Wow! :>1 month ago
- In general, the centroid of …1 month 1 week ago
- isn't the centroid of the…1 month 1 week ago
- I get it now, for long I was…1 month 3 weeks ago
- Why is BD Tension?
is it not…1 month 3 weeks ago - Bakit po nagmultiply ng 3/4…3 months 2 weeks ago
- Determine the least depth…1 year 1 month ago


I think of two versions of
I think of two versions of that problem.
1.) I got to get the derivative of $\sin(at)$ first before getting the Laplace transform of the derivative of $\sin(at).$
2.) This form: $\mathcal L\{ \frac{d}{dt}(sin (at)) \}$
I think I go do the #1.......because there is another operation that deas with Laplace transforms of derivatives.
Well...to get the derivative
To get the Laplace transform of derivative of $\sin (at)$, get first the derivative of $\sin (at)$. So we let $u = at$ and $du = a.$ Then recall that $\frac{d}{dx}(\sin u) = \cos(u) du$. So....
$$\frac{d}{dx}(\sin u ) = \cos (u) du$$ $$\frac{d}{dx}(\sin (at) ) = \cos (at) (a)$$ $$\frac{d}{dx}(\sin (at) ) = a \cos (at) $$
We will get the Laplace transform of $a \cos (at)$.
Recall that the Laplace transform of $\cos (\omega_o t)$ is $\frac{s}{s^2 + \omega_o ^2}$. Then the Laplace transform of $a \cos (at)$ would be:
$$\mathcal L \{ \cos (\omega_o t) \} = \frac{s}{s^2 + \omega_o ^2}$$ $$\mathcal L \{ a \cos (at) \} = a \left( \frac{s}{s^2 + (a)^2} \right)$$ $$\mathcal L \{ a \cos (at) \} = a \left( \frac{s}{s^2 + a^2} \right)$$
We conclude that Laplace transform of $a \cos (at)$ is $ \frac{a s}{s^2 + a^2} $.
Hope it helps:-)
hi Lee:-)
In reply to Well...to get the derivative by fitzmerl duron
hi Lee:-)