4. It turns out that the most general function that satisfies the equation is y Asin ot + Bcos ot, it is called the general solution. Because A and B are arbitrary constants we need two additional pieces of information to specify the displacement function completely. The most commonly specified conditions are the initial displacement and initial velocity of the block, y(0) and y'(0), respectively. Now let's look at the more realistic case in which frictional forces are present. Consider the case in which a=2 and e 2. Verify by substitution that the general solution is y e"(Acos 31+Bsin 31); that is, it satisfies the equation y"(t)+ay'(t)+wy(t)=0, for arbitrary constants A and B.

Advanced Engineering Mathematics
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ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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I would appreciate it if someone could help walk me through this part of #4.  

4. It turns out that the most general function that satisfies the equation is y Asin ot + Bcos ot,
it is called the general solution. Because A and B are arbitrary constants we need two additional pieces of
information to specify the displacement function completely. The most commonly specified conditions are
the initial displacement and initial velocity of the block, y(0) and y'(0), respectively.
Now let's look at the more realistic case in which frictional forces are present. Consider the case in which
a=2 and e 2. Verify by substitution that the general solution is y e"(Acos 31+Bsin 31);
that is, it satisfies the equation y"(t)+ay'(t)+wy(t)=0, for arbitrary constants A and B.
Transcribed Image Text:4. It turns out that the most general function that satisfies the equation is y Asin ot + Bcos ot, it is called the general solution. Because A and B are arbitrary constants we need two additional pieces of information to specify the displacement function completely. The most commonly specified conditions are the initial displacement and initial velocity of the block, y(0) and y'(0), respectively. Now let's look at the more realistic case in which frictional forces are present. Consider the case in which a=2 and e 2. Verify by substitution that the general solution is y e"(Acos 31+Bsin 31); that is, it satisfies the equation y"(t)+ay'(t)+wy(t)=0, for arbitrary constants A and B.
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