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.
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Method used for separation of mixture of products (B and C) obtained in the following reaction is: 