Question #225438

Question:

A particle moves such that its vector is given by 𝑟

= cos 𝜔𝑡𝑖 + sin 𝜔𝑡𝑗 where 𝜔 is a constant. Show that:

(i)

Velocity, 𝑣

of the particle is perpendicular to 𝑟


(ii)

Acceleration, 𝑎

is directed towards the origin and has magnitude proportional to the

distance from the origin.

(iii) 𝑟

𝑋 𝑣

is a constant vector


Expert's answer

The position vector is given by, r=cosωti^+sinωtj^\vec{r}=cos\omega t \hat{i}+sin\omega t \hat{j}


(a) Velocity is given by,

v=ddtr=ddt(cosωti^+sinωtj^)=ωsinωti^+ωcosωtj^\vec{v}= \frac{d}{dt}\vec{r}=\frac{d}{dt}(cos\omega t \hat{i}+sin\omega t \hat{j}) = -\omega sin\omega t \hat{i}+\omega cos\omega t \hat{j}

If velocity is perpendicular to position then, r.v=0\vec{r}.\vec{v} = 0

r.v=(cosωti^+sinωtj^).(ωsinωti^+ωcosωtj^)\vec{r}.\vec{v} = (cos\omega t \hat{i}+sin\omega t \hat{j}).(-\omega sin\omega t \hat{i}+\omega cos\omega t \hat{j})

r.v=ωsinωtcosωt+ωsinωtcosωt=0\vec{r}.\vec{v} = -\omega sin\omega t cos\omega t+\omega sin\omega t cos\omega t = 0

So, velocity and position are perpendicular.


(b) a=ddtv=ddt(ωsinωti^+ωcosωtj^)=ω2cosωti^ω2sinωtj^=ω2r\vec{a} = \frac{d}{dt} \vec{ v } =\frac{d}{dt}( -\omega sin\omega t \hat{i}+\omega cos\omega t \hat{j}) = -\omega^2 cos\omega t\hat{i} -\omega^2 sin\omega t\hat{j} = -\omega^2 \vec{r}

A negative sign indicates that it is acting toward the origin.

a=ω2r    ar|\vec{a}| = \omega^2|\vec{r}| \implies |\vec{a}| \propto|\vec{r}|


(c) r×v=(cosωti^+sinωtj^)×(ωsinωti^+ωcosωtj^)\vec{r} \times \vec{v} = (cos\omega t \hat{i}+sin\omega t \hat{j}) \times ( -\omega sin\omega t \hat{i}+\omega cos\omega t \hat{j})

r×v=(ωcos2ωt+ωsin2ωt)k^=ωk^\vec{r} \times \vec{v} = (\omega cos^2\omega t+ \omega sin^2\omega t)\hat{k} = \omega \hat{k}

Hence, it is a constant vector.




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