What is the hyperfocal distance for a 16-35mm landscape lens at f/11?
On a 16-35mm full-frame zoom at f/11, hyperfocal distance runs from roughly 0.82 meters at the 16mm wide end to roughly 3.90 meters at the 35mm long end — more than a fourfold range within one lens, purely from zooming across its own focal-length span.
Why the Wide End Does Most of the Work
At 16mm f/11, focusing at 0.82m already puts everything from about 0.41m to infinity in acceptably sharp focus — close enough to the camera that a nearby foreground rock or plant sits comfortably within the sharp zone without careful measurement. At 35mm, the same f/11 pushes the near limit out to 1.95m, a meaningfully less forgiving margin if your composition has anything closer than that in frame.
What This Means for Composing Across the Zoom Range
A composition built around a very close foreground element generally favors the wide end of this lens specifically because of how much shorter its hyperfocal distance runs — the same shot recomposed at 35mm might need a narrower aperture, a different focus point, or acceptance that the closest element won't read fully sharp. This is a real, practical reason landscape photographers often default toward the wider end of a 16-35mm rather than treating the whole range as interchangeable.
Check the exact figure at any focal length in this range in the DoF & Hyperfocal Calculator, pre-filled at 16mm f/11.
Frequently Asked Questions
Should I always shoot a 16-35mm at its widest end for landscapes?
Not always — the wide end gives the most forgiving hyperfocal distance, but 35mm's more restrained field of view and reduced edge distortion are often the better compositional choice when the scene doesn't need the most extreme wide angle available.
Does f/11 stay diffraction-safe across this whole zoom range?
Diffraction is a function of aperture and sensor pixel density, not focal length, so f/11 carries essentially the same diffraction risk at 16mm as it does at 35mm on the same camera — the hyperfocal-distance difference between the two ends comes entirely from focal length, not from any change in diffraction behavior.