Step 1: Keep everything in radians from the start.
Rather than switching between degrees and radians midway, convert the angle of attack range to radians up front and carry the calculation through in radians.
Step 2: Convert the section lift slope and the angle of attack change to radians.
$a_0 = 0.106 \times (180/\pi) = 6.073$ per radian (same as before).
$\Delta\alpha = \alpha - \alpha_{L0} = 3.5^{\circ}-(-1.5^{\circ}) = 5^{\circ} = 5 \times \dfrac{\pi}{180} = 0.0873$ rad.
Step 3: Apply the finite-wing correction.
$\pi e AR = \pi \times 0.95 \times 10 = 29.845$.
$a = \dfrac{a_0}{1+a_0/(\pi e AR)} = \dfrac{6.073}{1+6.073/29.845} = \dfrac{6.073}{1.2035} = 5.046$ per radian.
Step 4: Multiply the finite-wing slope by the angle change, both in radians.
$c_l = a \times \Delta\alpha = 5.046 \times 0.0873 = 0.4405$.
Final Answer:
Rounded to 2 decimal places, $c_l \approx 0.44$, matching the degree-based calculation.
\[ \boxed{c_l \approx 0.44} \]