Ignore air resistance. Consider a knuckleball with lateral motion satisfying the initial value problem x’’(t) = -25 sin (4ωt + θ0), x’(0) = x(0) = 0. Whit θ0 = 0 and ω = 1, find an equation for x(t) and graph the solution for 0 ≤ t ≤ 0.68. (HINT: Use integration by subtitution)
\[x''(t)=-25\sin(4\omega t+\theta_0)\] With the initial conditions \(x'(0)=x(0)=0\). Also, you're given actual values of \(\omega\) and \(\theta_0\), so you have the differential equation \[x''(t)=-25\sin(4t)\] Integrate both side with respect to \(t\): \[\int x''(t)~dt=\int-25\sin(4t)~dt\\ x'(t)=-25\left(\cdots\right)+C_1\] Integrate again: \[\int x'(t)~dt=\int\left[-25\left(\cdots\right)+C_1\right]~dt\\ x(t)=\cdots\] I'll let you fill in the blanks. Your general solution will have some constants, \(C_1\) and \(C_2\). You solve for these using the initial values.
ok
would that be 16 in the blanks?
@SithsAndGiggles
@SithsAndGiggles
\[\begin{align*}x'(t)&=\int(-25\sin(4t))~dt\\ &=-25\int\sin(4t)~dt\\ &=-25\left(-\frac{1}{4}\cos(4t)+C_1\right)\\ &=\frac{25}{4}\cos(4t)+C_1 \end{align*}\] Integrate both sides again, and you have \(x(t)=\cdots\). Now, use \(x'(0)=0\): \[x'(0)=0=\frac{25}{4}\cos(4\cdot0)+C_1~\Rightarrow~C_1=-\frac{25}{4}\] Do the same with \(x(0)=0\) to solve for \(C_2\) in \(x(t)=\cdots\).
@rizwan_uet can u help?
i already did what sith told me and i got x(t) = 25/16 sin(4t) for the first part..but i dont get when he said do the same with x(0) = 0 to solve for c2 in (t)
ok let me check
so what you got when you integrated it again???
i got 25/16 sin(4t) + c1
isnt it become x(t)= 25/16 sin(4t) + c2 ????? you put c1 here but its c2 actualy
ohhh ok
puting x(0) = 0 in this equation now you can get c2 thus 0 = 25/16sin(4x0) +c2
ohhh okay i see.
thanks
you are welcome
Join our real-time social learning platform and learn together with your friends!