In the travelling plane wave equation given by \( y = A \sin \omega \left( \frac{x}{v} - t \right) \), where \( \omega \) is the angular velocity and \( v \) is the linear velocity.
The dimension of \( \omega t \) is:
We are given the equation for the travelling wave as: \[ y = A \sin \omega \left( \frac{x}{v} - t \right) \] where \( y \) is the displacement, \( A \) is the amplitude, \( \omega \) is the angular velocity, \( v \) is the linear velocity, \( x \) is the position, and \( t \) is time.
We need to find the dimensions of \( \omega t \).
Step 1: The general dimension formula for angular velocity \( \omega \) is: \[ {Dimension of } \omega = \frac{{Dimension of angular displacement}}{{Dimension of time}} = \frac{{L}^0 {M}^0 {T}^0}{{T}} = {T}^{-1}. \] Step 2: The dimension of time \( t \) is simply: \[ {Dimension of } t = {T}. \] Step 3: Thus, the product \( \omega t \) has the dimension: \[ {Dimension of } \omega t = {T}^{-1} \times {T} = {T}^0. \] Therefore, the dimension of \( \omega t \) is \( {L}^0 {M}^0 {T}^0 \).
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: