We know:
\[ v_{\text{max}} = \omega A \quad \text{at mean position} \]
\[ \omega = \frac{2\pi}{T} \quad \text{and} \quad v_{\text{max}} = \frac{2\pi}{T} \times A \]
\[ v_{\text{max}} = \frac{2\pi}{3.14} \times 0.06 = 0.12 \, \text{m/s} \]
\[ v_{\text{max}} = 12 \, \text{cm/s} \]
This problem asks for the maximum velocity of a particle undergoing Simple Harmonic Motion (SHM). We are provided with the amplitude and the time period of the motion. The final answer needs to be expressed in cm/s.
For a particle executing Simple Harmonic Motion, its velocity \(v\) at any displacement \(x\) from the mean position is given by:
\[ v = \omega \sqrt{A^2 - x^2} \]where \(A\) is the amplitude and \(\omega\) is the angular frequency. The velocity is maximum when the particle is at its mean position, i.e., when \(x = 0\). The formula for the maximum velocity (\(v_{\text{max}}\)) is therefore:
\[ v_{\text{max}} = A\omega \]The angular frequency \(\omega\) is related to the time period \(T\) by the formula:
\[ \omega = \frac{2\pi}{T} \]Step 1: Identify the given values and convert them to the required units.
Amplitude, \(A = 0.06 \text{ m}\).
Since the final answer is required in cm/s, we convert the amplitude to cm:
\[ A = 0.06 \text{ m} \times 100 \frac{\text{cm}}{\text{m}} = 6 \text{ cm} \]Time period, \(T = 3.14 \text{ s}\).
Step 2: Calculate the angular frequency (\(\omega\)).
The value of the time period is given as 3.14 s, which is a good approximation for \(\pi\). So, we can take \(T \approx \pi\) s.
\[ \omega = \frac{2\pi}{T} \]Substituting the value of T:
\[ \omega = \frac{2\pi}{3.14 \text{ s}} \approx \frac{2\pi}{\pi \text{ s}} = 2 \text{ rad/s} \]Step 3: Calculate the maximum velocity (\(v_{\text{max}}\)) using the formula \(v_{\text{max}} = A\omega\).
Substitute the values of amplitude \(A\) (in cm) and angular frequency \(\omega\):
\[ v_{\text{max}} = (6 \text{ cm}) \times (2 \text{ rad/s}) \]Performing the multiplication gives the maximum velocity:
\[ v_{\text{max}} = 12 \text{ cm/s} \]The maximum velocity of the particle is 12 cm/s.
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,


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 : \(A_2 \rightleftharpoons 2A\)