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Date: 24-5-2018
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Date: 26-12-2018
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Date: 30-5-2018
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(1) |
find the first-order solution using a perturbation method. Write
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(2) |
and plug back into (1) and group powers to obtain
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(3) |
To solve this equation, keep terms only to order and note that, because this equation must hold for all powers of
, we can separate it into the two simultaneous differential equations
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(4) |
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(5) |
Setting our clock so that , the solution to (4) is then
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(6) |
Plugging this solution back into (5) then gives
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(7) |
The equation can be solved to give
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(8) |
Combining and
then gives
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(9) |
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(10) |
where the sinusoidal and cosinusoidal terms of order (from the
) have been ignored in comparison with the larger terms from
.
As can be seen in the top figure above, this solution approximates only for
. As the lower figure shows, the differences from the unperturbed oscillator grow stronger over time for even relatively small values of
.
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دخلت غرفة فنسيت ماذا تريد من داخلها.. خبير يفسر الحالة
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ثورة طبية.. ابتكار أصغر جهاز لتنظيم ضربات القلب في العالم
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قسم الشؤون الفكرية يعزز مكتبته بفهارس المخطوطات التركية
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