| Final exam: Wednesday, March 22, 7-10pm in PCYNH 109.  Bring ID! Last Quiz 4: Today (last one) Today: 11.12 Applications of Taylor Polynomials Next; Differential Equations | 
This section is about an example in the theory of relativity.  Let  be the (relativistic) mass of an object and
be the (relativistic) mass of an object and  be the mass at rest
(rest mass) of the object.  Let
 be the mass at rest
(rest mass) of the object.  Let  be the velocity of the object relative to the
observer, and let
 be the velocity of the object relative to the
observer, and let  be the speed of light.  These three quantities
are related as follows:
 be the speed of light.  These three quantities
are related as follows:
 (relativistic) mass
   (relativistic) mass
 :
:
 
 ?
?
Notice that
![$\displaystyle mc^2 - m_0 c^2 = \frac{m_0c^2}{\sqrt{1-\frac{v^2}{c^2}}} - m_0 c^2
= m_0 c^2 \left[ \left(1 - \frac{v^2}{c^2}\right)^{-\frac{1}{2}} - 1\right].
$](img1297.png) 
 
Let's compute the Taylor series  of  . We have
. We have
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![[*]](/usr/share/latex2html/icons/crossref.png) ):
):
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And we can ignore the higher order terms if 
 is small.
But how small is ``small'' enough, given that
 is small.
But how small is ``small'' enough, given that 
 appears
in an infinite sum?
 appears
in an infinite sum?