By definition of parsec
∴ 1 parsec =\((\frac{1AU}{1arc\,sec})\)
1 deg = 3600 arc sec
∴ 1 parsec = \(\frac{\pi}{3600\times180}\)radians
∴ 1 parsec = \(\frac{3600\times180}{\pi}\)AU
= 206265AU ≈ 2 × 105 AU
(b) At 1 AU distance, sun is (1/2) in diameter.
Therefore, at 1 parsec, star is \(\frac{1/2}{2\times 10^5}\) degree in diameter = 0.25 × 10-5 arc min
With 100 magnification, it should look 0.25 × 10-3 arc min. however, due to atmospheric fluctuations, it will still look of about 1 arc min.
∴ It can’t be magnified using telescope.
(c) \(\frac{D_{mars}}{D_{earth}}=\frac{1}{2},\)
\(\frac{D_{earth}}{D_{sun}}=\frac{1}{100}\)[Here, D = diameter]
\(\frac{D_{sun}}{D_{moon}}=400,\)
\(\frac{D_{earth}}{D_{moon}}=4\)
⇒ \(\frac{D_{mars}}{D_{sun}}=\frac{1}{2}\times\frac{1}{100}\)
At 1 AU sun is seen as ½ degree in diameter, and mars will be seen as 1/400 degree in diameter, i.e. mars diameter = \(\frac{1}{2}\times\frac{1}{200}=\frac{1}{400}\) at ½ AU. Mars diameter = \(\frac{1}{400}\times2°=(\frac{1}{200})°\)
At ½ AU mars will be seen as 1/400 degree in diameter. With 100 magnification mars will be seen mars diameter
=\(\frac{1°}{200}\times100=(\frac{1}{2})°=30\)
This is larger than resolution limit due to atmospheric fluctuations. Hence, it looks magnified.