Daniel B. answered 05/03/21
A retired computer professional to teach math, physics
Let's define
g(x) = x² + bx + 1
Then
g'(x) = 2x + b
g"(x) = 2
and
f(x) = ln(g(x))
Let's calculate the first and second derivative of f
f(x) = ln(g(x))
f'(x) = g'(x)/g(x)
f"(x) = g"(x)/g(x) - (g'(x))²/(g(x))²
a)
f has a stationary point for those x where
f(x) is defined, i.e. g(x) > 0 (1) and
f'(x) = 0, i.e., g'(x)/g(x) = 0 (2)
(2) simplifies into
g'(x) = 0
2x + b = 0
x = -b/2
Therefore f has a stationary point for those b where x = -b/2 satisfies (1)
g(-b/2) > 0
(-b/2)² + b(-b/2) + 1 > 0
b²/4 - b²/2 + 1 > 0
b² < 4
-2 < b < 2
S = {b | -2 < b < 2}
b)
Inflexion points are those values of x where
f(x) is defined, see (1), and
f"(x) = 0 (3)
First expand, simplify, and solve (3):
g"(x)/g(x) - (g'(x))²/(g(x))² = 0
g"(x)g(x) - (g'(x))² = 0
2(x² + bx + 1) - (2x + b)² = 0
2x² + 2bx + 2 - 4x² - 4xb - b² = 0
x² + bx + b²/2 - 1 = 0 (4)
x = (-b ± √(b² - 4(b²/2 - 1)))/2 = (-b ± √(4-b²))/2
That yields two distinct solutions provided 4-b² > 0,
which simplifies to
-2 < b < 2 (5)
Secondly any potential inflection point (i.e., any x satisfying (4)) must satisfy (1), which expands into
x² + bx + 1 > 0
That can be rewritten as
x² + bx + b²/2 - 1 - (b²/2 - 1) + 1 > 0
Using (4) this simplifies into
-(b²/2 - 1) + 1 > 0
That is simplifies into (5)
T = {b | -2 < b < 2}