Let H (t, x, p) be a Hamiltonian function that is convex in p. Let the associated Lagrangian satisfy the nonstandard minorization condition L(t, x, v) ≥ 1 2 m(|v| 2 −ω 2 |x| 2 )−C where m > 0, ω > 0, and C ≥ 0 are constants. Under some additional conditions, we prove that the associated value function is the unique viscosity solution of S t +H (t, x, ∇S) = 0 in Q T = (0, T )×R n , S| t=0 = S 0 , without any conditions at infinity on the solution.Here ωT < π/2. To the Hamilton-Jacobi equation corresponding to the classical action integrand in mechanics, we adjoin the continuity equation and establish the existence and uniqueness of a viscosity-measure solution (S, ρ) ofThis system arises in the WKB method. The measure solution is defined by means of the Filippov flow of ∇S.