“…[20]. The resulting global C 1 -smoothness of the spaces then enables the solution of fourth order PDEs just via its weak form using a standard Galerkin discretization, see for example [4,15,24,28,41,49] for the biharmonic equation, [3,6,32,33,34] for the Kirchhoff-Love shell formulation, [18,19,36] for the Cahn-Hilliard equation and [17,43] for plane problems of first strain gradient elasticity.…”