To find the value of a + b + m a+b+m a + b + m , we evaluate the given limit:
lim x → 2 sin ( x 3 − 5 x 2 + a x + b ) ( x − 1 − 1 ) log e ( x − 1 ) = m \lim _{x \rightarrow 2} \frac{\sin \left(x^3-5 x^2+a x+b\right)}{(\sqrt{x-1}-1) \log _e(x-1)}=m lim x → 2 ( x − 1 − 1 ) l o g e ( x − 1 ) s i n ( x 3 − 5 x 2 + a x + b ) = m
Let x = 2 + h x = 2 + h x = 2 + h . As x → 2 x \to 2 x → 2 , h → 0 h \to 0 h → 0 .
Step 1: Analyze the Denominator
The denominator becomes:
D ( h ) = ( 1 + h − 1 ) log e ( 1 + h ) D(h) = (\sqrt{1+h}-1) \log_e(1+h) D ( h ) = ( 1 + h − 1 ) log e ( 1 + h )
Using standard expansions as h → 0 h \to 0 h → 0 :
1 + h − 1 = h 1 + h + 1 = h 2 + O ( h 2 ) \sqrt{1+h} - 1 = \frac{h}{\sqrt{1+h} + 1} = \frac{h}{2} + O(h^2) 1 + h − 1 = 1 + h + 1 h = 2 h + O ( h 2 )
log e ( 1 + h ) = h + O ( h 2 ) \log_e(1+h) = h + O(h^2) log e ( 1 + h ) = h + O ( h 2 )
Therefore, the denominator behaves as:
D ( h ) = ( h 2 + O ( h 2 ) ) ( h + O ( h 2 ) ) = h 2 2 + O ( h 3 ) D(h) = \left(\frac{h}{2} + O(h^2)\right)\left(h + O(h^2)\right) = \frac{h^2}{2} + O(h^3) D ( h ) = ( 2 h + O ( h 2 ) ) ( h + O ( h 2 ) ) = 2 h 2 + O ( h 3 )
Since D ( h ) → 0 D(h) \to 0 D ( h ) → 0 as h → 0 h \to 0 h → 0 , for the limit m m m to exist and be finite, the numerator must also approach 0 0 0 .
Step 2: Determine a a a and b b b
Let P ( x ) = x 3 − 5 x 2 + a x + b P(x) = x^3 - 5x^2 + ax + b P ( x ) = x 3 − 5 x 2 + a x + b .
For sin ( P ( x ) ) → 0 \sin(P(x)) \to 0 sin ( P ( x )) → 0 as x → 2 x \to 2 x → 2 , we require:
P ( 2 ) = 0 P(2) = 0 P ( 2 ) = 0
Substitute x = 2 x = 2 x = 2 :
P ( 2 ) = 2 3 − 5 ( 2 ) 2 + 2 a + b = 8 − 20 + 2 a + b = 2 a + b − 12 = 0 ⟹ 2 a + b = 12 — (1) P(2) = 2^3 - 5(2)^2 + 2a + b = 8 - 20 + 2a + b = 2a + b - 12 = 0 \implies 2a + b = 12 \quad \text{--- (1)} P ( 2 ) = 2 3 − 5 ( 2 ) 2 + 2 a + b = 8 − 20 + 2 a + b = 2 a + b − 12 = 0 ⟹ 2 a + b = 12 — (1)
Since the denominator is of order h 2 h^2 h 2 , for the limit to be finite, P ( 2 + h ) P(2+h) P ( 2 + h ) must also be of order h 2 h^2 h 2 . Writing the Taylor expansion of P ( 2 + h ) P(2+h) P ( 2 + h ) around h = 0 h=0 h = 0 :
P ( 2 + h ) = P ( 2 ) + P ′ ( 2 ) h + P ′ ′ ( 2 ) 2 ! h 2 + … P(2+h) = P(2) + P'(2)h + \frac{P''(2)}{2!}h^2 + \dots P ( 2 + h ) = P ( 2 ) + P ′ ( 2 ) h + 2 ! P ′′ ( 2 ) h 2 + …
Since P ( 2 ) = 0 P(2) = 0 P ( 2 ) = 0 , we must also have the coefficient of h h h equal to 0 0 0 (i.e., P ′ ( 2 ) = 0 P'(2) = 0 P ′ ( 2 ) = 0 ).
Differentiating P ( x ) P(x) P ( x ) :
P ′ ( x ) = 3 x 2 − 10 x + a P'(x) = 3x^2 - 10x + a P ′ ( x ) = 3 x 2 − 10 x + a
Evaluating at x = 2 x = 2 x = 2 :
P ′ ( 2 ) = 3 ( 2 ) 2 − 10 ( 2 ) + a = 12 − 20 + a = a − 8 = 0 ⟹ a = 8 P'(2) = 3(2)^2 - 10(2) + a = 12 - 20 + a = a - 8 = 0 \implies a = 8 P ′ ( 2 ) = 3 ( 2 ) 2 − 10 ( 2 ) + a = 12 − 20 + a = a − 8 = 0 ⟹ a = 8
Substitute a = 8 a = 8 a = 8 into equation (1):
2 ( 8 ) + b = 12 ⟹ 16 + b = 12 ⟹ b = − 4 2(8) + b = 12 \implies 16 + b = 12 \implies b = -4 2 ( 8 ) + b = 12 ⟹ 16 + b = 12 ⟹ b = − 4
Step 3: Evaluate the Limit m m m
With a = 8 a = 8 a = 8 and b = − 4 b = -4 b = − 4 , the polynomial is:
P ( x ) = x 3 − 5 x 2 + 8 x − 4 = ( x − 2 ) 2 ( x − 1 ) P(x) = x^3 - 5x^2 + 8x - 4 = (x-2)^2(x-1) P ( x ) = x 3 − 5 x 2 + 8 x − 4 = ( x − 2 ) 2 ( x − 1 )
In terms of h = x − 2 h = x - 2 h = x − 2 :
P ( 2 + h ) = h 2 ( 2 + h − 1 ) = h 2 ( 1 + h ) P(2+h) = h^2(2+h-1) = h^2(1+h) P ( 2 + h ) = h 2 ( 2 + h − 1 ) = h 2 ( 1 + h )
Now we substitute this back into the limit:
m = lim h → 0 sin ( h 2 ( 1 + h ) ) ( 1 + h − 1 ) log e ( 1 + h ) m = \lim_{h \to 0} \frac{\sin\left(h^2(1+h)\right)}{(\sqrt{1+h}-1) \log_e(1+h)} m = lim h → 0 ( 1 + h − 1 ) l o g e ( 1 + h ) s i n ( h 2 ( 1 + h ) )
We rewrite the expression as:
m = lim h → 0 ( sin ( h 2 ( 1 + h ) ) h 2 ( 1 + h ) ) ⋅ ( h 2 ( 1 + h ) ( 1 + h − 1 ) log e ( 1 + h ) ) m = \lim_{h \to 0} \left( \frac{\sin\left(h^2(1+h)\right)}{h^2(1+h)} \right) \cdot \left( \frac{h^2(1+h)}{(\sqrt{1+h}-1) \log_e(1+h)} \right) m = lim h → 0 ( h 2 ( 1 + h ) s i n ( h 2 ( 1 + h ) ) ) ⋅ ( ( 1 + h − 1 ) l o g e ( 1 + h ) h 2 ( 1 + h ) )
Using the standard limit lim y → 0 sin y y = 1 \lim_{y \to 0} \frac{\sin y}{y} = 1 lim y → 0 y s i n y = 1 :
m = 1 ⋅ lim h → 0 1 + h ( 1 + h − 1 h ) ( log e ( 1 + h ) h ) m = 1 \cdot \lim_{h \to 0} \frac{1+h}{\left(\frac{\sqrt{1+h}-1}{h}\right) \left(\frac{\log_e(1+h)}{h}\right)} m = 1 ⋅ lim h → 0 ( h 1 + h − 1 ) ( h l o g e ( 1 + h ) ) 1 + h
Applying the standard limits:
lim h → 0 1 + h − 1 h = 1 2 \lim_{h \to 0} \frac{\sqrt{1+h}-1}{h} = \frac{1}{2} lim h → 0 h 1 + h − 1 = 2 1
lim h → 0 log e ( 1 + h ) h = 1 \lim_{h \to 0} \frac{\log_e(1+h)}{h} = 1 lim h → 0 h l o g e ( 1 + h ) = 1
Thus:
m = 1 + 0 1 2 ⋅ 1 = 2 m = \frac{1+0}{\frac{1}{2} \cdot 1} = 2 m = 2 1 ⋅ 1 1 + 0 = 2
Step 4: Calculate a + b + m a+b+m a + b + m
a + b + m = 8 + ( − 4 ) + 2 = 6 a + b + m = 8 + (-4) + 2 = 6 a + b + m = 8 + ( − 4 ) + 2 = 6