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Uncertainty

From Luter 345 Experiments
Revision as of 17:59, 24 December 2024 by Brash99 (talk | contribs) (1 revision imported)
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Variable Definitions[edit | edit source]

$ l\rightarrow $ length of pendulum
$ g\rightarrow $ gravity
$ T\rightarrow $ period of the pendulum
$ \delta T\rightarrow $ uncertainty in the period
$ \delta g\rightarrow $ uncertainty in the gravity
$ \delta l\rightarrow $ uncertainty in the length

Uncertainty in the Measurement of g[edit | edit source]

The theory section shows that $ g $ is found to be:

$ g={\frac {4\pi ^{2}l}{T^{2}}} $

From this, the error can be found by:

$ \left({\frac {\delta g}{g}}\right)^{2}=\left({\frac {\delta l}{l}}\right)^{2}+\left(2{\frac {\delta T}{T}}\right)^{2} $

This formulation is then used for calculations of the uncertainty and the accuracy necessary for keeping the error withing 1/10000. The error on the period is found from:

$ \delta T={\frac {\sigma }{\sqrt {N}}} $

where:

$ \sigma ={\sqrt {{\frac {1}{N-1}}\sum \limits _{i=1}^{N}\left(T_{i}-{\bar {T}}\right)^{2}}} $