Step 1: Outside a charged conducting sphere, the field is the same as if all its charge were concentrated at the centre:
\[E = \frac{1}{4\pi\epsilon_0}\,\frac{q}{r^2} = \frac{k\,q}{r^2}\]
Step 2: Rearrange to find the charge, using \(k = 9\times10^{9}\,\text{N m}^2\,\text{C}^{-2}\):
\[q = \frac{E\,r^2}{k}\]
Step 3: Substitute \(E = 1.5\times10^{3}\,\text{N C}^{-1}\) and \(r = 20\,\text{cm} = 0.20\,\text{m}\):
\[q = \frac{(1.5\times10^{3})\times(0.20)^2}{9\times10^{9}}\]
Step 4: Do the arithmetic:
\[q = \frac{(1.5\times10^{3})\times(0.04)}{9\times10^{9}} = \frac{60}{9\times10^{9}} = 6.67\times10^{-9}\,\text{C}\]
Step 5: Fix the sign. The field points radially inward (toward the centre), which happens only for a negative charge. So:
\[q = -6.67\times10^{-9}\,\text{C} = -6.67\,\text{nC}\]
The radius of the sphere (10 cm) is not needed because the field point lies outside it.
\[\boxed{q = -6.67\,\text{nC}}\]