For \( \alpha, \beta, \gamma \in \mathbb{R} \), if \[ \lim_{x \to 0} \frac{x^2 \sin(\alpha x) + (\gamma - 1)e^{x^2}}{\sin(2x - \beta x)} = 3, \] then \( \beta + \gamma - \alpha \) is equal to:
We are asked to find the value of \( \beta + \gamma - \alpha \) for \( \alpha, \beta, \gamma \in \mathbb{R} \), given the following limit:
\[ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2}}{\sin 2x - \beta x} = 3 \]To solve this limit problem, we will use the Maclaurin series (Taylor series expansion around \(x=0\)) for the functions involved. The key series expansions are:
The limit is in the indeterminate form \( \frac{0}{0} \). For the limit to result in a finite, non-zero constant, the lowest power of \( x \) in the numerator's series expansion must be the same as the lowest power of \( x \) in the denominator's expansion.
Step 1: Determine the value of \( \gamma \).
As \( x \to 0 \), the denominator \( D(x) = \sin 2x - \beta x \to \sin(0) - \beta(0) = 0 \). For the limit to be finite, the numerator \( N(x) \) must also approach 0.
\[ \lim_{x \to 0} \left( x^2 \sin \alpha x + (\gamma - 1)e^{x^2} \right) = 0^2 \sin(0) + (\gamma - 1)e^0 = 0 + (\gamma - 1)(1) = \gamma - 1 \]Setting the numerator to 0:
\[ \gamma - 1 = 0 \implies \gamma = 1 \]Step 2: Expand the numerator and denominator using Maclaurin series.
With \( \gamma = 1 \), the numerator becomes:
\[ N(x) = x^2 \sin(\alpha x) \]Using the expansion for \( \sin(\alpha x) \):
\[ N(x) = x^2 \left( \alpha x - \frac{(\alpha x)^3}{3!} + \dots \right) = \alpha x^3 - \frac{\alpha^3 x^5}{6} + \dots \]The denominator is:
\[ D(x) = \sin(2x) - \beta x \]Using the expansion for \( \sin(2x) \):
\[ D(x) = \left( 2x - \frac{(2x)^3}{3!} + \dots \right) - \beta x = (2 - \beta)x - \frac{8x^3}{6} + \dots = (2 - \beta)x - \frac{4}{3}x^3 + \dots \]Step 3: Determine the value of \( \beta \).
The limit expression is now:
\[ \lim_{x \to 0} \frac{\alpha x^3 - \frac{\alpha^3 x^5}{6} + \dots}{(2 - \beta)x - \frac{4}{3}x^3 + \dots} = 3 \]The lowest power of \( x \) in the numerator is \( x^3 \). For the limit to be a finite, non-zero value, the lowest power of \( x \) in the denominator must also be \( x^3 \). This means the coefficient of the lower power term (\(x\)) in the denominator must be zero.
\[ 2 - \beta = 0 \implies \beta = 2 \]Step 4: Determine the value of \( \alpha \).
After setting \( \beta = 2 \), the limit becomes:
\[ \lim_{x \to 0} \frac{\alpha x^3 - \frac{\alpha^3 x^5}{6} + \dots}{-\frac{4}{3}x^3 + \dots} = 3 \]We can evaluate this limit by taking the ratio of the coefficients of the lowest power terms (\(x^3\)):
\[ \frac{\alpha}{-\frac{4}{3}} = 3 \] \[ \alpha = 3 \times \left(-\frac{4}{3}\right) = -4 \]We have found the values of the parameters:
Now, we compute the required expression \( \beta + \gamma - \alpha \):
\[ \beta + \gamma - \alpha = 2 + 1 - (-4) = 3 + 4 = 7 \]Thus, the value of \( \beta + \gamma - \alpha \) is 7.
If $\lim_{x \to 1} \frac{(x-1)(6+\lambda \cos(x-1)) + \mu \sin(1-x)}{(x-1)^3} = -1$, where $\lambda, \mu \in \mathbb{R}$, then $\lambda + \mu$ is equal to
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:
The major product (A) formed in the following reaction sequence is
