To solve the given equation \(e^{\sin x} - 2e^{-\sin x} = 2\), let's first introduce a substitution. Let \(y = e^{\sin x}\). Then \(e^{-\sin x} = \frac{1}{y}\). Substituting these into the equation gives:
\(y - 2\left(\frac{1}{y}\right) = 2\)
Multiplying through by \(y\) to clear the fraction, we get:
\(y^2 - 2 = 2y\)
Rearrange the equation:
\(y^2 - 2y - 2 = 0\)
Now, we solve this quadratic equation using the quadratic formula, \(y = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), where \(a = 1\), \(b = -2\), and \(c = -2\).
\(y = \frac{2 \pm \sqrt{(-2)^2 - 4 \cdot 1 \cdot (-2)}}{2 \cdot 1}\)
\(y = \frac{2 \pm \sqrt{4 + 8}}{2}\)
\(y = \frac{2 \pm \sqrt{12}}{2}\)
\(y = \frac{2 \pm 2\sqrt{3}}{2}\)
\(y = 1 \pm \sqrt{3}\)
Thus, the potential solutions for \(y\) are \(1 + \sqrt{3}\) and \(1 - \sqrt{3}\). However, since \(y = e^{\sin x}\), which is always a positive number (as the exponential function is always positive), \(1 - \sqrt{3}\) is not possible because it is negative.
Let's analyze the feasible solution:
For \(y = 1 + \sqrt{3}\), we have:
\(e^{\sin x} = 1 + \sqrt{3}\)
This implies \(\sin x = \ln(1 + \sqrt{3})\). However, the range of the sine function is \([-1, 1]\), and \(\ln(1 + \sqrt{3})\) is greater than 1. Therefore, it is not possible for \(\sin x\) to equal \(\ln(1 + \sqrt{3})\).
As there is no valid solution that satisfies the original equation, the number of solutions is 0.
Rewrite the equation:
\[ e^{\sin x} - 2e^{-\sin x} = 2. \]
Let \( y = e^{\sin x} \). Then \( e^{-\sin x} = \frac{1}{y} \), and the equation becomes:
\[ y - \frac{2}{y} = 2. \]
Multiply both sides by \( y \) to clear the denominator:
\[ y^2 - 2 = 2y. \]
Rearrange terms:
\[ y^2 - 2y - 2 = 0. \]
This is a quadratic equation in \( y \):
\[ y = \frac{2 \pm \sqrt{4 + 8}}{2} = \frac{2 \pm \sqrt{12}}{2} = 1 \pm \sqrt{3}. \]
Since \( y = e^{\sin x} \) and \( e^{\sin x} > 0 \), we discard \( y = 1 - \sqrt{3} \) (as it is negative) and consider \( y = 1 + \sqrt{3} \).
However, for \( y = e^{\sin x} = 1 + \sqrt{3} \), we need \( \sin x = \ln(1 + \sqrt{3}) \). Since \( \ln(1 + \sqrt{3}) \) exceeds the range of \( \sin x \) (which is \([-1, 1]\)), there is no value of \( x \) that satisfies this equation.
Conclusion: There are no solutions.
Thus, the answer is: 0
Given:
Take \( e^{\sin x} = t \) where \( t > 0 \).
Step 1: Solve for \( t \):
We start by solving the equation: \[ t - \frac{2}{t} = 2 \] Multiplying both sides by \( t \): \[ t^2 - 2 = 2t \] Rearranging the terms: \[ t^2 - 2t - 2 = 0 \] \[ t^2 - 2t + 1 = 3 \] Factoring the quadratic: \[ (t - 1)^2 = 3 \] Taking the square root of both sides: \[ t - 1 = \pm \sqrt{3} \] Solving for \( t \): \[ t = 1 \pm 1.73 \] This gives two possible values for \( t \): \[ t = 2.73 \quad \text{or} \quad t = -0.73 \] Since \( t > 0 \), we reject \( t = -0.73 \).
Step 2: Solve for \( \sin x \):
We now have: \[ e^{\sin x} = 2.73 \] Taking the natural logarithm of both sides: \[ \ln e^{\sin x} = \ln 2.73 \] Simplifying: \[ \sin x = \log_e 2.73 \] Using a calculator: \[ \sin x = 1.0 \]
Conclusion:
Since \( \sin x = 1 \), this means that there is no solution for \( x \) because the value of \( \sin x \) cannot exceed 1. Therefore, there is no solution.
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,