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Maximum mass loss of steel was found to occur at the centre of the corrosion region.
Also, the maximum mass loss values were obtained at non-swirling regime and low angles of incidence.
The values of maximum mass loss rate decreased roughly with increasing filler weight fraction, while the influence of the filler diameter and length diameter ratio on the maximum mass loss rate was insignificant.
Each sample's top value among maximum mass loss rates of all reaction stages appears during reaction 4 stage.
A maximum mass loss of steel of 1% was found to reduce the flexural capacity of beams by 0.7%.
By adding 5.0 wt% f-BN nanosheets, the maximum mass loss rate, peak heat release rate (pHRR), and smoke produce rate (SPR) were decreased by 20.8 %, 68.0%, and 53.6%, respectively.
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Also, there are obvious differences among SARA fractions in combustion temperature range, maximum thermal mass loss temperature, mass loss percentage and mass loss rate in each combustion stage.
The ultimate flexural capacity of beams was found to be best related to the maximum gravimetric mass loss compared to the average mass loss of steel.
Corresponding thermogravimetric data are summarized in Table 2, where the temperatures at which 5% (T 5%), 50% (T 50%), and maximum (T max) mass loss occur are described as the initial degradation temperature, half degradation temperature, and maximum degradation temperature, respectively.
The numerical factor (f_{mathrm{wind}}) establishes a maximum average of 1% mass loss from stellar winds per timestep.
Consequently, this shift in the mass loss maxima suggests more defects and disorders for the nitrogen-doped MWNTs which are in good agreement with the Raman results.
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