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PreprintCC BY 4.0Zenodo

A Discrete-Time Summation Derivation of the Second Equation of Motion

  1. 1Independent Researcher

Abstract

The second equation of motion, s = ut + ½at², is usually derived by integrating velocity or from the area under a velocity-time graph. This paper presents an alternative, calculus-free derivation based on summing the displacement covered in successive unit-time intervals. Assuming constant acceleration and using the velocity at the start of each interval, the total displacement is found to be s = ut + ½at² − ½at. The extra term −½at is shown to be a discretisation error caused by ignoring the change of velocity within each interval. Generalising to a time step h gives s = ut + ½at² − ½ath, which reduces to the standard equation as h → 0. Using the mid-interval velocity removes the error exactly. The method gives students an elementary, summation-based explanation of where the factor ½ in ½at² comes from and links kinematics to the idea of Riemann sums.

Independent student research. This preprint has not been peer-reviewed. An AI assistant was used to check the algebra and help with writing.

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BibTeX
@misc{asthana2026discretetime,
  title = {{A Discrete-Time Summation Derivation of the Second Equation of Motion}},
  author = {Amritanshu Asthana},
  howpublished = {Zenodo},
  year = {2026},
  month = oct,
  doi = {10.5281/zenodo.23657193},
  url = {https://zenodo.org/records/23657193},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - A Discrete-Time Summation Derivation of the Second Equation of Motion
AU  - Amritanshu Asthana
PY  - 2026
DA  - 2026/10/26
PB  - Zenodo
DO  - 10.5281/zenodo.23657193
UR  - https://zenodo.org/records/23657193
AB  - The second equation of motion, s = ut + ½at², is usually derived by integrating velocity or from the area under a velocity-time graph. This paper presents an alternative, calculus-free derivation based on summing the displacement covered in successive unit-time intervals. Assuming constant acceleration and using the velocity at the start of each interval, the total displacement is found to be s = ut + ½at² − ½at. The extra term −½at is shown to be a discretisation error caused by ignoring the change of velocity within each interval. Generalising to a time step h gives s = ut + ½at² − ½ath, which reduces to the standard equation as h → 0. Using the mid-interval velocity removes the error exactly. The method gives students an elementary, summation-based explanation of where the factor ½ in ½at² comes from and links kinematics to the idea of Riemann sums.  Independent student research. This preprint has not been peer-reviewed. An AI assistant was used to check the algebra and help with writing.
ER  -