The position vector is given by, r ⃗ = c o s ω t i ^ + s i n ω t j ^ \vec{r}=cos\omega t \hat{i}+sin\omega t \hat{j} r = cos ω t i ^ + s inω t j ^
(a) Velocity is given by,
v ⃗ = d d t r ⃗ = d d t ( c o s ω t i ^ + s i n ω t j ^ ) = − ω s i n ω t i ^ + ω c o s ω t j ^ \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} v = d t d r = d t d ( cos ω t i ^ + s inω t j ^ ) = − ω s inω t i ^ + ω cos ω t j ^
If velocity is perpendicular to position then, r ⃗ . v ⃗ = 0 \vec{r}.\vec{v} = 0 r . v = 0
r ⃗ . v ⃗ = ( c o s ω t i ^ + s i n ω t j ^ ) . ( − ω s i n ω t i ^ + ω c o s ω t j ^ ) \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 = ( cos ω t i ^ + s inω t j ^ ) . ( − ω s inω t i ^ + ω cos ω t j ^ )
r ⃗ . v ⃗ = − ω s i n ω t c o s ω t + ω s i n ω t c o s ω t = 0 \vec{r}.\vec{v} = -\omega sin\omega t cos\omega t+\omega sin\omega t cos\omega t = 0 r . v = − ω s inω t cos ω t + ω s inω t cos ω t = 0
So, velocity and position are perpendicular.
(b) a ⃗ = d d t v ⃗ = d d t ( − ω s i n ω t i ^ + ω c o s ω t j ^ ) = − ω 2 c o s ω t i ^ − ω 2 s i n ω t j ^ = − ω 2 r ⃗ \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 = d t d v = d t d ( − ω s inω t i ^ + ω cos ω t j ^ ) = − ω 2 cos ω t i ^ − ω 2 s inω t j ^ = − ω 2 r
A negative sign indicates that it is acting toward the origin.
∣ a ⃗ ∣ = ω 2 ∣ r ⃗ ∣ ⟹ ∣ a ⃗ ∣ ∝ ∣ r ⃗ ∣ |\vec{a}| = \omega^2|\vec{r}| \implies |\vec{a}| \propto|\vec{r}| ∣ a ∣ = ω 2 ∣ r ∣ ⟹ ∣ a ∣ ∝ ∣ r ∣
(c) r ⃗ × v ⃗ = ( c o s ω t i ^ + s i n ω t j ^ ) × ( − ω s i n ω t i ^ + ω c o s ω t j ^ ) \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 = ( cos ω t i ^ + s inω t j ^ ) × ( − ω s inω t i ^ + ω cos ω t j ^ )
r ⃗ × v ⃗ = ( ω c o s 2 ω t + ω s i n 2 ω t ) k ^ = ω k ^ \vec{r} \times \vec{v} = (\omega cos^2\omega t+ \omega sin^2\omega t)\hat{k} = \omega \hat{k} r × v = ( ω co s 2 ω t + ω s i n 2 ω t ) k ^ = ω k ^
Hence, it is a constant vector.