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QJEEAdv22Ph82f8: JEE Advanced 2022 Physics - Class 11 JEEAdv22Ph82f8 Solution: A particle of mass is subjected to a force which depends on the …

A particle of mass 1 kg1 \mathrm{~kg} is subjected to a force which depends on the position as F⃗=\vec{F}= −k(xı^+yȷ^)kg ms−2-k(x \hat{\imath}+y \hat{\jmath}) \mathrm{kg}\, \mathrm{m} \mathrm{s}^{-2} with k=1 kg s−2k=1 \mathrm{~kg} \mathrm{~s}^{-2} . At time t=0t=0 , the particle's position r⃗=\vec{r}= (12ı^+2ȷ^)m\left(\frac{1}{\sqrt{2}} \hat{\imath}+\sqrt{2} \hat{\jmath}\right) m and its velocity v⃗=(−2ı^+2ȷ^+2πk^)ms−1\vec{v}=\left(-\sqrt{2} \hat{\imath}+\sqrt{2} \hat{\jmath}+\frac{2}{\pi} \hat{k}\right) m s^{-1} . Let vxv_{x} and vyv_{y} denote the xx and the yy components of the particle's velocity, respectively. Ignore gravity. When z=0.5 mz=0.5 \mathrm{~m} , the value of (xvy−yvx)\left(x v_{y}-y v_{x}\right) is __________ m2s−1m^{2} s^{-1} .

Step-by-Step Verified Solution

Fx=−x=maxF_x=-x=m a_x

So ax=d2xdt2=−xa_x=\frac{d^2 x}{d t^2}=-x

⇒x=Axsin⁡(ωt+ϕx)(ω=1rad/s)\Rightarrow x=A_x \sin \left(\omega t+\phi_x\right) \quad(\omega=1 \mathrm{rad} / \mathrm{s})

and vx=Axωcos⁡(ωt+ϕx)v_x=A_x \omega \cos \left(\omega t+\phi_x\right)

at t=0,x=12 mt=0, x=\frac{1}{\sqrt{2}} \mathrm{~m} and vx=−2 m/sv_x=-\sqrt{2} \mathrm{~m} / \mathrm{s}

So 12=Axsin⁡ϕx\frac{1}{\sqrt{2}}=A_x \sin \phi_x

and −2=Axcos⁡ϕx-\sqrt{2}=A_x \cos \phi_x

amp;⇒tan⁡ϕx=−12......(1)amp; and Ax=52 m......(2)\begin{aligned}& \Rightarrow \tan \phi_x=-\frac{1}{2} ......(1) \\& \text { and } A_x=\sqrt{\frac{5}{2}} \mathrm{~m} ......(2)\end{aligned}

Similarly

amp;Fy=−y=may.amp;⇒d2ydt2=−y\begin{aligned}& F_y=-y=m a_y . \\\\& \Rightarrow \frac{d^2 y}{d t^2}=-y\end{aligned}

So, y=Aysin⁡(ωt+ϕy)(ω=1rad/s)y=A_y \sin \left(\omega \mathrm{t}+\phi_{\mathrm{y}}\right) \quad(\omega=1 \mathrm{rad} / \mathrm{s}) and

vy=Ayωcos⁡(ωt+ϕy)v_y=A_y \omega \cos \left(\omega t+\phi_y\right)

at t=0,y=2 mt=0,y=\sqrt{2} \mathrm{~m} and vy=2 m/sv_y=\sqrt{2} \mathrm{~m} / \mathrm{s}

So 2=Aysin⁡ϕ\sqrt{2}=A_y \sin \phi

and 2=Aycos⁡ϕ\sqrt{2}=A_y \cos \phi

⇒ϕ=π4 and Ay=2\Rightarrow \phi=\frac{\pi}{4} \text { and } A_y=2

So,

(xvy−yvx)\left(x v_y-y v_x\right)

=52sin⁡(ωt+ϕx)×2cos⁡(ωt+ϕy)−2sin⁡(ωt+ϕy)×52cos⁡(ωt+ϕx)=\sqrt{\frac{5}{2}} \sin \left(\omega t+\phi_x\right) \times 2 \cos \left(\omega t+\phi_y\right)-2 \sin \left(\omega t+\phi_y\right) \times \sqrt{\frac{5}{2}} \cos \left(\omega t+\phi_x\right)

=52×2(sin⁡(ωt+ϕx)cos⁡(ωt+ϕy)−sin⁡(ωt+ϕy)×cos⁡(ωt+ϕx)=\sqrt{\frac{5}{2}} \times 2\left(\sin \left(\omega t+\phi_x\right) \cos \left(\omega t+\phi_y\right)-\sin \left(\omega t+\phi_y\right) \times \cos \left(\omega t+\phi_x\right)\right.

=10sin⁡(ϕx−ϕy)=\sqrt{10} \sin \left(\phi_x-\phi_y\right)

=10(sin⁡ϕxcos⁡ϕy−cos⁡ϕxsin⁡ϕy)=\sqrt{10}\left(\sin \phi_x \cos \phi_y-\cos \phi_x \sin \phi_y\right)

=10(15×12−(−25)×12)=\sqrt{10}\left(\frac{1}{\sqrt{5}} \times \frac{1}{\sqrt{2}}-\left(-\frac{2}{\sqrt{5}}\right) \times \frac{1}{\sqrt{2}}\right)

=3=3

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