If $$f(x) = \begin{cases} 2 \sin x & \text{for} \ -\pi \leq x \leq -\frac{\pi}{2}, a \sin x + b & \text{for} \ -\frac{\pi}{2}<x<\frac{\pi}{2}, \cos x & \text{for} \ \frac{\pi}{2} \leq x \leq \pi,\end{cases}$$and it is continuous on $[- \pi, \pi]$, then the values of $ a $ and $ b $ are:
To determine the values of \( a \) and \( b \) that make the function \( f(x) \) continuous at \( x = \pm\frac{\pi}{2} \), we analyze the continuity conditions at these points.
1. Continuity at \( x = \frac{\pi}{2} \):
The function changes definition at \( \frac{\pi}{2} \). We examine both sides:
Left-hand limit (LHL):
\[ \lim_{x \to \pi/2^-} (a \sin x + b) = a \sin\left(\frac{\pi}{2}\right) + b = a + b \]
Right-hand limit (RHL):
\[ \lim_{x \to \pi/2^+} \cos x = \cos\left(\frac{\pi}{2}\right) = 0 \]
For continuity, LHL = RHL:
\[ a + b = 0 \quad \text{(Equation 1)} \]
2. Continuity at \( x = -\frac{\pi}{2} \):
The function also changes definition at \( -\frac{\pi}{2} \):
Left-hand limit (LHL):
\[ \lim_{x \to -\pi/2^-} 2 \sin x = 2 \sin\left(-\frac{\pi}{2}\right) = -2 \]
Right-hand limit (RHL):
\[ \lim_{x \to -\pi/2^+} (a \sin x + b) = a \sin\left(-\frac{\pi}{2}\right) + b = -a + b \]
For continuity, LHL = RHL:
\[ -a + b = -2 \quad \text{(Equation 2)} \]
3. Solving the System of Equations:
From Equation 1: \( b = -a \)
Substitute into Equation 2:
\[ -a + (-a) = -2 \Rightarrow -2a = -2 \Rightarrow a = 1 \]
Then \( b = -1 \)
Final Answer:
The values that make \( f(x) \) continuous are \( a = 1 \) and \( b = -1 \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: