If lim⁡x→1(x−1)(6+λcos⁡(x−1))+μsin⁡(1−x)(x−1)3=−1\lim_{x\to1} \frac{(x-1)(6 + \lambda \cos(x-1)) + \mu \sin(1-x)}{(x-1)^3} = -1 where λ,μ∈R\lambda, \mu \in \mathbb{R} then λ+μ\lambda + \mu is equal to:

Answer: 18

Step-by-step solution

Step 1: Substitute t=x−1t = x-1

To simplify the limit expression, we introduce a substitution. Let t=x−1t = x-1. As xx approaches 11, tt approaches 00. This transformation makes the limit easier to evaluate using standard Maclaurin series expansions.

Step 2: Rewrite the limit in terms of tt

After substituting t=x−1t = x-1, the expression becomes t(6+λcos⁡(t))+μsin⁡(−t)t3\frac{t(6 + \lambda \cos(t)) + \mu \sin(-t)}{t^3}. We also use the property that sin⁡(−t)=−sin⁡(t)\sin(-t) = -\sin(t).

Step 3: Apply Maclaurin series expansions

We use the Maclaurin series expansions for cos⁡(t)=1−t22!+t44!−…\cos(t) = 1 - \frac{t^2}{2!} + \frac{t^4}{4!} - \dots and sin⁡(t)=t−t33!+t55!−…\sin(t) = t - \frac{t^3}{3!} + \frac{t^5}{5!} - \dots. We only need terms up to t3t^3 in the numerator to match the denominator.

Step 4: Simplify the expression

Expand the terms in the numerator and group them by powers of tt. This helps us identify the coefficients of tt and t3t^3.

Step 5: Equate coefficients to solve for λ\lambda and μ\mu

For the limit to be finite and non-zero, the coefficient of tt in the numerator must be zero. This gives us 6+λ−μ=06 + \lambda - \mu = 0. Then, the limit becomes the coefficient of t3t^3, so μ6−λ2=−1\frac{\mu}{6} - \frac{\lambda}{2} = -1.

Step 6: Solve the system of equations

Substitute the first equation into the second: (λ+6)−3λ=−6(\lambda + 6) - 3\lambda = -6. This simplifies to −2λ=−12-2\lambda = -12, so λ=6\lambda = 6. Then, μ=6+6=12\mu = 6 + 6 = 12.

Step 7: Calculate λ+μ\lambda + \mu

Finally, we calculate the sum of λ\lambda and μ\mu using the values we found.

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