The Taylor series for ex, cosx, and e−x around x=0 are:
eax=1+ax+2!(ax)2+…, cos(bx)=1−2!(bx)2+…, e−cx=1−cx+2!(cx)2−…. Substituting these into the limit and simplifying:
x→0lim1−cos2x(1+ax+2!(ax)2)−(1−2!(bx)2)−2cx(1−(cx)+2!(cx)2). This simplifies to:
x→0lim((2x)21−cos2x)×4x2(a−2c)x+(2a2+b2+c2)x2+…. Let's evaluate this expression:
((2x)21−cos2x)×4x2. We know that 1−cos2x can be rewritten using the double-angle formula for cosine, which is cos2x=1−2sin2x.
So, 1−cos2x=2sin2x.
Substituting this into our expression we get:
((2x)22sin2x)×4x2. This simplifies to:
(xsinx)2×4x2=21×4x2=2x2. So,
((2x)21−cos2x)×4x2=2x2. ∴
x→0lim2x2(a−2c)x+(2a2+b2+c2)x2+…=17. Now, for the limit to exist, the coefficient of x in the numerator must be zero, as the limit would be undefined otherwise.
This gives us the equation:
a−2c=0⇒c=2a. Then, for the limit to equal 17, the coefficient of x2 in the numerator must equal 17×2=34.
This gives us the equation:
2a2+b2+c2=34⇒a2+b2+c2=68. Since c=2a, we can substitute c in the equation to get:
a2+b2+(2a)2=68⇒5a2+b2=68.