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But I must explain to you how all this mistaken idea of denouncing of a pleasure and praising pain was born and I will give you a complete account of the system, and expound the actual teachings of the great explorer of the truth. No one rejects, dislikes, or avoids pleasure itself, because it is pleasure Bik 2009, but because those who do not know how to pursue pleasure rationally encounter consequences that are extremely painful. Nor again is there anyone Pepe 2012 who loves or pursues or desires to obtain pain of itself, because it is pain, but occasionally circumstances occur in which toil and pain can procure him some great pleasure. To take a trivial example, which of us ever undertakes laborious physical exercise, except to obtain some advantage from it? But who has any right to find fault with a man who chooses to enjoy a pleasure that has no annoying consequences, or one who avoids a pain that produces no resultant pleasure?

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Most amazinf figure ever Ganz 2014       
On the other hand, we denounce with righteous indignation and dislike men who are so beguiled and demoralized by the charms of pleasure of the moment, so blinded by desire, \(e=mc^2+\beta\gamma\frac{\sqrt{s}}{r^3}\)that they cannot foresee Wong 2016 the pain and trouble that are bound to ensue; and equal blame belongs to those who fail in their duty through weakness of will, which is the same as saying through shrinking from toil and pain. These cases are perfectly simple and easy to distinguish. In a free hour, when our power  of choice is untrammeled and when nothing prevents our being able to do what we like best, every pleasure is to be welcomed and every pain avoided. But in certain circumstances and owing to the claims of duty or the obligations of business it will frequently occur that pleasures have to be repudiated and annoyances accepted. The wise man therefore always holds in these matters to this principle of selection: he rejects pleasures to secure other greater pleasures, or else he endures pains to avoid worse pains.

We now utilize the same method presented in to calculate expected visibilities of both dipole and quadrupole modes in stars with \(1.25 \, M_\odot \leq M \leq 3 \, M_\odot\). The ratio of suppressed mode power to normal mode power is \[\label{eqn:vsup} \frac{V_{\rm sup}^2}{V_{\rm norm}^2} = \bigg[ 1 + \Delta \nu \,\tau \,T^2 \bigg]^{-1} \, .\] Here, \(\Delta \nu\) is the large frequency separation, \(\tau\) is the radial mode lifetime, and \(T\) is the wave transmission coefficient through the evanescent zone. The value of \(T\) can be calculated via \[\label{eqn:T} T = \exp \bigg[ - \int^{r_2}_{r_1} dr \sqrt{ - \frac{ \big( L_\ell^2 - \omega^2 \big) \big(N^2 - \omega^2 \big) }{v_s^2 \omega^2} } \bigg] \, .\]

References

  1. Holly M. Bik. Unravelling post-glacial colonization through molecular techniques: new insight from estuarine invertebrates. Journal of Biogeography 36, 16–17 Wiley-Blackwell, 2009. Link

  2. Alberto Pepe, Matthew S. Mayernik. The Use of Microblogging for Field-Based Scientific Research. In 2012 45th Hawaii International Conference on System Sciences. Institute of Electrical & Electronics Engineers (IEEE), 2012. Link

  3. Holly Ganz, Jonathan Eisen, Leesa Li, Ruth Lee, David Coil, Katie Dahlhausen, Holly Bik. Microbial resistance to disinfectants in animal shelters. ThinkLab, 2014. Link

  4. JY Wong, W Zhang, D Kargbo, U Haque, W Hu, P Wu, A Kamara, Y Chen, B Kargbo, GE Glass, R Yang, BJ Cowling, C Liu. Assessment of the severity of Ebola virus disease in Sierra Leone in 2014-2015.. Epidemiol Infect 144, 1473-81 (2016).

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