\(\alpha^2 + \beta^2 + \gamma^2 = 6\)
\(\alpha \beta + \beta \gamma + \gamma \alpha + 1 = 0\)
\(\alpha \beta^2 + \beta \gamma^2 + \gamma \alpha^2 + 3 = 0\)
\(\alpha^2 - \beta^2 + \gamma^2 = 4\)
Let's solve the given limit problem and determine which option is NOT correct. We are given:
\(\lim_{{x \to 0}} \frac{\alpha e^x + \beta e^{-x} + \gamma \sin x}{x \sin^2 x} = \frac{2}{3}\)
To evaluate this limit, we begin by expanding the terms in the numerator and the denominator as \(x\) approaches 0 using Taylor series expansions:
Substitute these expansions into our limit expression:
\(\frac{\alpha(1 + x + \frac{x^2}{2}) + \beta(1 - x + \frac{x^2}{2}) + \gamma(x - \frac{x^3}{6})}{x(x^2 - \frac{x^4}{3})}\)
Simplify the numerator:
\((\alpha + \beta) + (\alpha - \beta + \gamma)x + \left(\frac{\alpha + \beta}{2}\right)x^2 + \ldots\)
The denominator simplifies to:
\((x^3 - \frac{x^5}{3})\)
We focus on the most significant terms as \(x\) approaches 0:
The dominant term in the denominator is \(x^3\), and hence for the limit to be non-zero (specifically, \(\frac{2}{3}\)), a cube term must arise from the numerator:
The expression becomes significant if:
\(\alpha - \beta + \gamma = 0\) (justifying coefficients of \(x\).)
If the coefficient of cubic term \((\frac{\alpha + \beta}{2})x^2\) ensures non-zero value:
Equating to \(\frac{2}{3}\):
\(\frac{\alpha + \beta}{2} = \frac{2}{3}\)
And \((\alpha - \beta + \gamma)\) adjusts any lower order non-zero terms.
Solving these equations systematically, assessing options:
Evaluate options:
Testing specific options for consistency and checking through derived equations.
Finally, evaluate each using computed relations, and determine inconsistencies. The incorrect option checked is:
\(\alpha \beta^2 + \beta \gamma^2 + \gamma \alpha^2 + 3 = 0\)
Hence, this is the option that is NOT correct.
\(\lim_{{x \to 0}} \frac{\alpha e^x + \beta e^{-x} + \gamma \sin x}{x \sin^2 x} = \frac{2}{3}\)
\(⇒ α + β = 0\) (to make indeterminant form) …(i)
Now,
\(\lim_{{x \to 0}} \frac{\alpha e^x + \beta e^{-x} + \gamma \sin x}{x \sin^2 x} = \frac{2}{3}\)
(Using L-H Rule)
\(⇒ α – β + γ = 0\) (to make indeterminant form) …(ii)
Now,
\(\lim_{{x \to 0}} \frac{\alpha e^x + \beta e^{-x} + \gamma \sin x}{6x} = \frac{2}{3}\)
(Using L-H Rule)
\(⇒\)\(\frac{\alpha - \beta - \gamma}{6} = \frac{2}{3}\)
\(⇒\)\(α – β – γ = 4 …(iii)\)
\(⇒\) \(γ = –2\)
and eq(i) + eq(ii)
\(2α = –γ\)
On solving,
\(⇒ α = 1\ \text{and}\ β = –1\)
and \(\alpha \beta^2 + \beta \gamma^2 + \gamma \alpha^2 + 3\)
\(= 1 – 4 – 2 + 3\)
\(= –2\)
So, the correct option is (C): \(\alpha \beta^2 + \beta \gamma^2 + \gamma \alpha^2 + 3 = 0\)
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,
A function's limit is a number that a function reaches when its independent variable comes to a certain value. The value (say a) to which the function f(x) approaches casually as the independent variable x approaches casually a given value "A" denoted as f(x) = A.
If limx→a- f(x) is the expected value of f when x = a, given the values of ‘f’ near x to the left of ‘a’. This value is also called the left-hand limit of ‘f’ at a.
If limx→a+ f(x) is the expected value of f when x = a, given the values of ‘f’ near x to the right of ‘a’. This value is also called the right-hand limit of f(x) at a.
If the right-hand and left-hand limits concur, then it is referred to as a common value as the limit of f(x) at x = a and denote it by lim x→a f(x).