Relativity 4#
Example 2: How Good is the Approximation?#
The Question:
Remember that the expansion of the gamma function that was used was $$
\[\begin{align*}
\gamma &=\frac{1}{\sqrt{{1-\beta^2}}} \\
\text{ the approximation is: } \gamma &\approx 1+\dfrac{1}{2}\beta^2
\end{align*}\]
\[ \begin{align}\begin{aligned}
How far out in speed must we go with the approximate expansion of the gamma function to deviate from the real value by 0.1?\\
------\\**The Answer:** \\Let's look at some values of $\beta$ and use the interactive $\gamma$ in the text and compare to the calculated approximation. For example:\\for $\beta = 0.2$, \end{aligned}\end{align} \]
\gamma \approx 1+ \frac{1}{2} (0.2)^2 = 1.02 \nonumber $$
Here’s a collection of comparisons:
\(\beta\) |
actual \(\gamma\) |
approx. \(\gamma\) |
---|---|---|
0.2 |
1.021 |
1.02 |
0.3 |
1.048 |
1.045 |
0.4 |
1.091 |
1.08 |
0.5 |
1.155 |
1.125 |
0.6 |
1.25 |
1.18 |
So by the time the speed has reached 60% of the speed of light, the approximation is no longer valid by about 0.1. One would then add another term in the expansion which would make the approximation: $\( \gamma \approx 1+ \frac{1}{2} \beta^2 + \frac{3}{8}\beta^4 \nonumber \)$ which would add 0.049 to the value in the table.