First, the equation of a circle centered at the origin p . O ( 0 ; 0 ) p.O\left(0;0\right) p . O ( 0 ; 0 ) and radius R = a > 0 R=a>0 R = a > 0 has the form
x 2 + y 2 = a 2 x^2+y^2=a^2 x 2 + y 2 = a 2
For example, a = 3 a=3 a = 3
Secondly, from physics we know the relationship between the velocity vector and the radius vector
r → = x ( t ) ⋅ i → + y ( t ) ⋅ j → ⟶ v → = d r → d t = d x ( t ) d t ⋅ i → + d y ( t ) d t ⋅ j → v → = v x ( t ) ⋅ i → + v y ( t ) ⋅ j → ⟶ ∣ v → ∣ = v x 2 + v y 2 \overrightarrow{r}=x(t)\cdot\overrightarrow{i}+y(t)\cdot\overrightarrow{j}\longrightarrow\\[0.3cm]
\overrightarrow{v}=\frac{d\overrightarrow{r}}{dt}=\frac{dx(t)}{dt}\cdot\overrightarrow{i}+\frac{dy(t)}{dt}\cdot\overrightarrow{j}\\[0.3cm]
\overrightarrow{v}=v_x(t)\cdot\overrightarrow{i}+v_y(t)\cdot\overrightarrow{j}\longrightarrow\\[0.3cm]
\left|\overrightarrow{v}\right|=\sqrt{v_x^2+v_y^2} r = x ( t ) ⋅ i + y ( t ) ⋅ j ⟶ v = d t d r = d t d x ( t ) ⋅ i + d t d y ( t ) ⋅ j v = v x ( t ) ⋅ i + v y ( t ) ⋅ j ⟶ ∣ ∣ v ∣ ∣ = v x 2 + v y 2
In our case, the natural variable t − t- t − time was replaced by the general variable s s s .
v → ≡ δ → ( s ) = ( a cos a s ) ⏟ δ x ( s ) ⋅ i → + ( a sin a s ) ⏟ δ y ( s ) ⋅ i → ⟶ ∣ δ → ( s ) ∣ = δ x 2 ( s ) + δ y 2 ( s ) = ( a cos a s ) 2 + ( a sin a s ) 2 = = a 2 ( cos 2 a s + sin 2 a s ) = a ⋅ 1 = a \overrightarrow{v}\equiv\overrightarrow{\delta}(s)=\underbrace{\left(a\cos as\right)}_{\delta_x(s)}\cdot\overrightarrow{i}+\underbrace{\left(a\sin as\right)}_{\delta_y(s)}\cdot\overrightarrow{i}\longrightarrow\\[0.3cm]
\left|\overrightarrow{\delta}(s)\right|=\sqrt{\delta_x^2(s)+\delta_y^2(s)}=\sqrt{\left(a\cos as\right)^2+\left(a\sin as\right)^2}=\\[0.3cm]
=\sqrt{a^2\left(\cos^2as+\sin^2as\right)}=a\cdot\sqrt{1}=a v ≡ δ ( s ) = δ x ( s ) ( a cos a s ) ⋅ i + δ y ( s ) ( a sin a s ) ⋅ i ⟶ ∣ ∣ δ ( s ) ∣ ∣ = δ x 2 ( s ) + δ y 2 ( s ) = ( a cos a s ) 2 + ( a sin a s ) 2 = = a 2 ( cos 2 a s + sin 2 a s ) = a ⋅ 1 = a
Conclusion,
∣ δ ( s ) → ∣ = { is a unit speed , if a = 1 is not a unit speed , if a ≠ 1 \left|\overrightarrow{\delta(s)}\right|=\left\{\begin{array}{l}
\text{is a unit speed},\quad\text{if}\quad a=1\\[0.3cm]
\text{is not a unit speed},\quad\text{if}\quad a\neq1
\end{array}\right. ∣ ∣ δ ( s ) ∣ ∣ = { is a unit speed , if a = 1 is not a unit speed , if a = 1