a particle moves according to the equation x=acosPi t the distance covered by it in 2.5 sec is
x=a*cos(pi*t) x=a*cos(2.5*pi)=?
answer is 5a -_-
x=a*cos(2*pi+0.5pi)=a*cos0.5*pi=a*0=?
Using the arclength formula and recognizing that \(\sin(\pi x)<0\) when \(1<x<2\) and positive otherwise in the interval \([0,2.5]\) $$ x(t)=a\cos\pi t\\ x'(t)={d\over dt}x(t)=-a\pi \sin\pi t\\ |x'(t)|=a\pi\sin \pi t \\ \text{Which means, }\\ a\pi\sin(x)=\left\{\begin{matrix} a\pi\sin(x)&0<x<1\\ -a\pi\sin(x)&1<x<2\\ a\pi\sin(x)&2<x<2.5\\ \end{matrix}\right.\\ \text{So, }\\ \int_0^{2.5}\left |x'(t)\right | dt=\int_0^{2.5}\left |a\pi \sin \pi t\right | dt\\ =a\pi\left ( \int_0^{1} \sin \pi t dt-\int_1^{2} \sin \pi t dt+\int_2^{2.5} \sin \pi t dt\right )\\ =a\pi\left (\left .{-cos\pi t\over \pi}\right |_0^1+\left .{cos\pi t\over \pi}\right |_1^2+\left .{-cos\pi t\over \pi}\right |_2^{2.5}\right)\\ =a\left ((-(-1)-(-1))+(1-(-1)-(0-1)\right)\\ =5a $$
Here is an interactive chart of your problem I've created for you - http://tube.geogebra.org/student/m843545 Let me know if you have any questions.
(Note that there may be a delay in the calculation of Arclength in the link above because the calculation is actually occurring out in a "cloud" server" - just wait a few seconds for the results)
(Note that there may be a delay in the calculation of Arclength in the link above because the calculation is actually occurring out in a "cloud" server" - just wait a few seconds for the results)
@ybarrap your math is actually calculating the area under the curve, not an **arc length**. in a proper arc length integral you would not need to split out the integration intervals in order to make the number work. in an arc length integration ds = sqrt ( x' ^ 2 + y' 2). @kittycat01 if you start with the thing this question really deals with, namely simple harmonic motion, you should see the answer below.|dw:1426463835536:dw| i will rip that picture again in the next post and highlight the distance thing as that seems to be the only way to show different colours..
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