The phrase "are small for all" is not correct and does not convey a clear meaning in written English.
It may be intended to describe something that is small in size for everyone, but the phrasing is awkward and unclear.
Example: "The shoes available in the store are small for all, making it difficult for customers to find their size."
Alternatives: "are small for everyone" or "are universally small".
The lots, which range from one and one-quarter to one and one-half acres, are small for all that must fit: patios, pools, circular driveways, play equipment and gazebos, as well as the house.
Within one type of dose calibrator, the deviations are small for all isotopes: the standard deviation for repeated measurements is below 3%, while the effect of varying syringes and vials is about 5-105-10%
The corresponding MAE and MSD results are small for all compared attributes, which indicates that the log-based attribute values are close to the values of the self-declared questionnaire attributes: Physical Attributes Frequency: The average difference between the user self-reported frequency and the one captured in logs is 0.88 days.
The PPVs are small for all three methods, which is probably due to the fact that only a small set of conditions was tested in the ChIP-chip experiments.
Standard deviations are small for all methods.
Relative standard deviations are small for all methods, although slightly larger for the direct method.
The average value of WAIT for this group falls by 10.72 0.87=9.85 min. The average value of DELAY falls by 4.70 0.76=3.94 min. Changes in WAIT and DELAY are smaller for all other groups.
Furthermore, when it occurs, it usually affects only a few grid cells, i.e., the residual is small for all the velocity components except in very localized regions.
The non-shared environmental contribution was greater with age for the Digit Span tests and Block Design, while the shared environmental component was small for all tests, often more so with age.
The inhomogeneous broadening value is small for all capping layers at room temperature, and it shows the increasing trend for Cr and Cu capping layers, increasing to 66 Oe and 28 Oe respectively with T an.
A Boussinesq method is derived that is fully dispersive, in the sense that the error of the approximation is small for all 0⩽kh<∞ (k the magnitude of the wave number and h the water depth).
