Concept:
When a block moves down an inclined plane without acceleration, it is moving with a constant velocity. This means the net force acting along the incline surface is zero, indicating that the downward component of gravity is perfectly balanced by the upward kinetic friction force ($mg \sin\theta = f_k = \mu_k mg \cos\theta$). This gives:
\[
\mu_k = \tan\theta
\]
When the angle of inclination is increased, a net driving force is established, and the resulting acceleration is given by Newton's second law:
\[
a = g(\sin\theta' - \mu_k \cos\theta')
\]
Step 1: Determine the coefficient of kinetic friction ($\mu_k$).
Given that the block slides at constant speed when $\theta = 30^\circ$:
\[
\mu_k = \tan(30^\circ) = \frac{1}{\sqrt{3}}
\]
Step 2: Calculate the acceleration at the new inclination angle.
The inclination is increased by $30^\circ$, making the new angle:
\[
\theta' = 30^\circ + 30^\circ = 60^\circ
\]
Substitute $\theta' = 60^\circ$, $\mu_k = \frac{1}{\sqrt{3}}$, and $g = 9.8\text{ m s}^{-2}$ into the acceleration equation:
\[
a = g\left(\sin(60^\circ) - \frac{1}{\sqrt{3}}\cos(60^\circ)\right)
\]
We know that $\sin(60^\circ) = \frac{\sqrt{3}}{2}$ and $\cos(60^\circ) = \frac{1}{2}$:
\[
a = g\left(\frac{\sqrt{3}}{2} - \frac{1}{\sqrt{3}}\cdot\frac{1}{2}\right) = g\left(\frac{\sqrt{3}}{2} - \frac{1}{2\sqrt{3}}\right)
\]
Find a common denominator inside the parentheses:
\[
a = g\left(\frac{3 - 1}{2\sqrt{3}}\right) = g\left(\frac{2}{2\sqrt{3}}\right) = \frac{g}{\sqrt{3}}
\]
Substituting $g = 9.8\text{ m s}^{-2}$ and $\sqrt{3} \approx 1.732$:
\[
a = \frac{9.8}{1.732} \approx 5.658\text{ m s}^{-2} \approx 5.66\text{ m s}^{-2}
\]