No your first diagram is correct. These types of problems treat light as rays, not waves.
Think back to Young's Double Slit Experiment
[tex]n\lambda = dsin(\theta)[/tex]
The right side of the equation solved for the path length difference between rays from the slits. In order for constructive interference to occur, the path length difference must equal an integer multiple of a wavelength (crests fall on crests). Similarly, destructive interference happened when the path length difference equaled an integer plus a half multiple of wavelength (0.5x, 1.5x, 2.5x...) (crests fall on troughs). However, notice in Young's Double Slit Experiment the light was coherent (in phase). In this problem the light is possibly not coherent as rays will undergo a 180 degree phase shift whenever they travel from a lower index of refraction to a higher index of refraction.
Notice in this case that the ray reflected from the top of the film has a 180 degree phase shift and the ray reflected from the bottom of the film also has a 180 degree phase shift. Therefore the two rays are actually for all intents and purposes in phase.
So the path length difference between the two rays (for near normal incidence) is 2t and this should therefore be equal to an integer plus a half times the wavelength of light for destructive interference. In other words,
[tex]2t = (n + \frac{1}{2})\lambda_{in film}[/tex]