Find y''_xx for the cycloid x = a (t- sin t), y = a (1
Find $y''_{xx}$ for the cycloid $x = a\bigl(t-\sin t\bigr),\ y = a\bigl(1-\cos t\bigr)$.
Explanation of Method
Half-angle identities turn the cycloid's slope into a cotangent.
Step 1: Derivatives with respect to $t$
\[ \dot x = a\bigl(1-\cos t\bigr), \qquad \dot y = a\sin t. \]
Step 2: First derivative, simplified by half angles
Using $\sin t = 2\sin\tfrac{t}{2}\cos\tfrac{t}{2}$ and $1-\cos t = 2\sin^{2}\tfrac{t}{2}$: \[y'_{x} = \frac{a\sin t}{a\bigl(1-\cos t\bigr)} = \frac{2\sin\tfrac{t}{2}\cos\tfrac{t}{2}}{2\sin^{2}\tfrac{t}{2}} = \cot\frac{t}{2}.\]
Step 3: Differentiate with respect to $t$
The inner derivative $\tfrac12$ appears as a factor: \[\bigl(y'_{x}\bigr)'_{t} = -\frac{1}{\sin^{2}\tfrac{t}{2}}\cdot\frac12 = -\frac{1}{2\sin^{2}\tfrac{t}{2}}.\]
Step 4: Divide by $\dot x$
Writing $\dot x = 2a\sin^{2}\tfrac{t}{2}$ again, the two squared sines combine into a fourth power: \[y''_{xx} = \frac{-\dfrac{1}{2\sin^{2}\tfrac{t}{2}}}{2a\sin^{2}\tfrac{t}{2}} = -\frac{1}{4a\sin^{4}\tfrac{t}{2}}.\]
Step 5: A neater form
The ordinate itself is $y = a\bigl(1-\cos t\bigr) = 2a\sin^{2}\tfrac{t}{2}$, so $\sin^{4}\tfrac{t}{2} = \dfrac{y^{2}}{4a^{2}}$ and
\[ y''_{xx} = -\frac{1}{4a}\cdot\frac{4a^{2}}{y^{2}} = -\frac{a}{y^{2}}. \]
The curvature of the cycloid is thus governed entirely by its height above the base line.
Step 6: Verification
\[t = \pi \text{ (top of the arch): } \sin\frac{\pi}{2} = 1 \;\Longrightarrow\; y''_{xx} = -\frac{1}{4a}\]
\[\text{From the neat form: } y = 2a \;\Longrightarrow\; -\frac{a}{4a^{2}} = -\frac{1}{4a} \;\;\checkmark\]
\[y''_{xx}\lt 0 \text{ for every } t\neq2k\pi: \text{ each arch is concave down throughout} \;\;\checkmark\]
Result
Final answer:
\[\boxed{\,y''_{xx} = -\dfrac{1}{4a\sin^{4}\dfrac{t}{2}}\,}\]
Remark
Remark. At $t = 2k\pi$ the point touches the base line, $y = 0$, and $y''_{xx}\to-\infty$: these are the cusps, where both $\dot x$ and $\dot y$ vanish and the curve has a vertical tangent. Between two cusps the arch is concave down everywhere, with its gentlest bending at the summit — which is the analytic form of the fact that the cycloid is the curve of fastest descent.