Step 1: Look at the top of the circle.
At the highest point, the string tension $T$ and the weight $mg$ both point downward, toward the centre of the vertical circle.
Step 2: Apply Newton's second law for circular motion.
The net inward force equals the centripetal requirement: \[ T + mg = \frac{mv^2}{r} \]
Step 3: Write down the data.
$m = 1$ kg, $r = 1$ m, $v = 4$ ms$^{-1}$, $g = 10$ ms$^{-2}$.
Step 4: Centripetal force needed.
$\dfrac{mv^2}{r} = \dfrac{1\times 16}{1} = 16$ N.
Step 5: Weight contribution.
$mg = 1\times 10 = 10$ N, which already supplies part of the inward force.
Step 6: Solve for the tension.
$T = 16 - 10 = 6$ N.
\[ \boxed{6\ \text{N}} \]