We are bounded in a nutshell of Infinite space: Blog Post #22, Worksheet # 7.1, Problem #6: All the light you can barely see
6. If your telescope can detect optical magnitudes \(m_V \leq 21\) how far away, in parsecs, can you detect a Type Ia supernova with your telescope? (HINT: The Sun’s absolute magnitude is \(M_V =4.83\) .)
Here, we’ll be going back to some of our earlier problems involving distance moduli and Luminosity and magnitude comparisons. From previous problems and known astronomical facts, we have:
\[L_{Ia} = 3.1308 \times 10^{43} \frac{ergs}{s} ,\] the luminosity of the sun is: \[L_\odot = 3.846 \times 10^{33} \frac{ergs}{s} ,\] and the equation for comparing absolute magnitudes is \[M_\star - M_\odot = -10^{0.4} \log_10 \left(\frac{L_\star}{L_\odot}\right) . \] Having these values, as well as the Absolute Magnitude of the sun, given by the problem, \(M_V =4.83\), then we can simply solve for the absolute magnitude of the Supernova. \[M_{Ia} - M_\odot = -10^{0.4} \log_{10} \left(\frac{L_{Ia}}{L_\odot}\right) ,\] \[M_{Ia}= -10^{0.4} \log_{10} \left(\frac{L_{Ia}}{L_\odot}\right) + M_\odot,\] \[M_{Ia}= -10^{0.4} \log_{10} \left(\frac{3.1308 \times 10^{43} \frac{ergs}{s}}{3.846 \times 10^{33} \frac{ergs}{s}}\right) + 4.83,\] \[ M_{Ia}= -24.8944 + 4.83,\] \[M_{Ia} = -20.061.\]
Now knowing the absolute magnitude of the supernova, we can now solve for the maximum distance when the max apparent magnitude that can be recorded is 21. Using \[m – M = 5 \log_{10} (d) -5 ,\] \[ d \leq 10^{\frac{m- M +5}{5}} ,\] \[ d\leq 10^{\frac{21- (-20.06) +5}{5}} ,\] \[ d\leq 10^{9.212} ,\] \[ d \leq 1.629 \times 10^ 9 pc = 1.629 \times 10^6 kpc ,\] which is the max distance our telescopes can see with present technology, for now.
This is pretty far! Though for reasonable exposure times our modern telescopes can actually see much farther than that (galaxies and stuff)!
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