Step 1: Start from the general law:
$\Delta U = q + w$, where $w$ is work done on the system.
Step 2: Apply the adiabatic condition:
Adiabatic means the system is thermally insulated, so $q = 0$. Then $\Delta U = w$.
Step 3: Match the options:
Negating both sides of $\Delta U = w$ gives $-\Delta U = -w$, which is option (B).
(A) $w = -q$ gives $\Delta U = 0$, which is true for an isothermal ideal gas, not an adiabatic change.
(C) $\Delta U = qV$ is not a recognised form of the law.
(D) keeps a heat term, so it cannot describe a process with no heat flow.
Final Answer:
Option (B) is the correct statement.
\[ \boxed{-\Delta U = -W \text{ (B)}} \]