- Rotational Period of the Sun = 28.3 days
- Angular Size of the Sun = 0.56$^{o}$
- Rotational Velocity of the Sun = 0.975 km/s
$P_\odot V_\odot = \boldsymbol{Circ}_\odot =2\pi R_\odot$
$R_\odot = \frac{P_\odot V_\odot}{2\pi}$
Now that we know the radius of the sun, we can use geometry to find the Astronomical Unit, d
where $\alpha = \frac{\theta}{2}$.
According to the picture above, $\tan(\alpha )=\frac{R_\odot}{d}$. Because of small angle approximation*, we can say that $\tan(\alpha ) = \alpha $, which leads us to the equation
$\alpha = \frac{\theta}{2}= \frac{R_\odot}{d}$
$d=\frac{2R_\odot}{\theta}$
When you substitute the radius equation for $R_\odot$, you get this equation for the Astronomical Unit:
$d=\frac{\frac{P_\odot V_\odot}{2\pi}}{\frac{\theta}{2}}=\frac{P_\odot V_\odot}{\pi \theta}$
Our group found that the distance to the sun is $7.986\times 10^{12}$ cm, which is about half the actual value. This makes sense because the rotational velocity we found was almost exactly half of the actual value.
*Small angle approximation says that, for $\theta < < 1^{o} $, $\sin \theta = \theta$ and $\cos \theta =1$
Hi Moiya,
ReplyDeleteYou covered the basics here, but it would be helpful to see a more detailed discussion of the result. Why do we care about measuring the AU? How would the measurement be improved?