We need to find the uniform velocity \( v_2 \) for the second part of a journey, given the distances traveled, the velocity for the first part \( v_1 \), and the average velocity for the entire journey.
The average velocity (\( v_{\text{avg}} \)) is defined as the total displacement divided by the total time taken. For motion in a straight line without a change in direction, the displacement is equal to the total distance.
\[ v_{\text{avg}} = \frac{\text{Total Distance}}{\text{Total Time}} \]
The total time is the sum of the time taken for each segment of the journey, where time \( t \) is calculated as \( t = \frac{\text{distance}}{\text{velocity}} \).
Step 1: Define the total distance traveled.
The person travels a distance \( d_1 = x \) with velocity \( v_1 \) and a distance \( d_2 = \frac{3x}{2} \) with velocity \( v_2 \).
The total distance is:
\[ D_{\text{total}} = d_1 + d_2 = x + \frac{3x}{2} = \frac{2x + 3x}{2} = \frac{5x}{2} \]
Step 2: Define the total time taken.
The time taken for the first part of the journey is \( t_1 = \frac{d_1}{v_1} = \frac{x}{v_1} \).
The time taken for the second part of the journey is \( t_2 = \frac{d_2}{v_2} = \frac{3x/2}{v_2} = \frac{3x}{2v_2} \).
The total time is:
\[ T_{\text{total}} = t_1 + t_2 = \frac{x}{v_1} + \frac{3x}{2v_2} \]
Step 3: Set up the equation for the average velocity.
\[ v_{\text{avg}} = \frac{D_{\text{total}}}{T_{\text{total}}} = \frac{\frac{5x}{2}}{\frac{x}{v_1} + \frac{3x}{2v_2}} \]
Step 4: Simplify the expression for average velocity.
We can factor out \( x \) from the denominator:
\[ v_{\text{avg}} = \frac{\frac{5x}{2}}{x \left( \frac{1}{v_1} + \frac{3}{2v_2} \right)} = \frac{\frac{5}{2}}{\frac{1}{v_1} + \frac{3}{2v_2}} \]
Now, find a common denominator for the terms in the bottom part:
\[ v_{\text{avg}} = \frac{\frac{5}{2}}{\frac{2v_2 + 3v_1}{2v_1v_2}} = \frac{5}{2} \times \frac{2v_1v_2}{3v_1 + 2v_2} = \frac{5v_1v_2}{3v_1 + 2v_2} \]
Step 5: Substitute the given values into the equation.
We are given \( v_{\text{avg}} = \frac{50}{7} \, \text{m/s} \) and \( v_1 = 5 \, \text{m/s} \).
\[ \frac{50}{7} = \frac{5(5)v_2}{3(5) + 2v_2} \] \[ \frac{50}{7} = \frac{25v_2}{15 + 2v_2} \]
Step 6: Solve the equation for \( v_2 \).
Divide both sides by 25:
\[ \frac{50}{7 \times 25} = \frac{v_2}{15 + 2v_2} \] \[ \frac{2}{7} = \frac{v_2}{15 + 2v_2} \]
Now, cross-multiply:
\[ 2(15 + 2v_2) = 7v_2 \] \[ 30 + 4v_2 = 7v_2 \] \[ 30 = 7v_2 - 4v_2 \] \[ 30 = 3v_2 \] \[ v_2 = \frac{30}{3} = 10 \]
The value of \( v_2 \) is 10 m/s.
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
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\(^{-2}\).
