Given Information:
- Displacement from \( t \) to \( t+1 \): \( \Delta x = 125 \, \text{m} \)
- Velocity increase from \( t \) to \( t+1 \): \( \Delta v = 50 \, \text{m/s} \)
Now, Calculate Acceleration:
Using the formula:
\(a = \frac{\Delta v}{\Delta t}\)
Substituting \( \Delta v = 50 \, \text{m/s} \) and \( \Delta t = 1 \, \text{s} \):
\(a = \frac{50}{1} = 50 \, \text{m/s}^2\)
Equation of Motion:
The formula for distance traveled in the \( n \)-th second is:
\(S_n = u + \frac{a}{2} (2n - 1)\)
Find Initial Velocity (\( u \)):
Distance traveled in the \( (t+1) \)-th second is \( S_{t+1} = 125 \, \text{m} \). Substituting \( n = 1 \), \( a = 50 \, \text{m/s}^2 \), and \( S_{t+1} = 125 \):
\(125 = u + \frac{50}{2}(2 \cdot 1 - 1)\)
Simplifying:
\(125 = u + 25\)
\(u = 125 - 25 = 100 \, \text{m/s}\)
Now, Calculate Distance for \( (t+2) \)-th Second:
Substituting \( u = 100 \, \text{m/s} \), \( a = 50 \, \text{m/s}^2 \), and \( n = 2 \) into the equation:
\(S_{t+2} = u + \frac{a}{2}(2 \cdot 2 - 1)\)
Simplifying:
\(S_{t+2} = 100 + \frac{50}{2}(3)\)
\(S_{t+2} = 100 + 25 \times 3\)
\(S_{t+2} = 100 + 75 = 175 \, \text{m}\)
\(\boxed{\text{The distance traveled in the } (t+2)\text{-th second is } 175 \, \text{m}.}\)
The problem asks for the distance travelled by a particle in the \((t+2)^{\text{th}}\) second, given its displacement and the increase in its velocity during the time interval from \(t\) to \((t+1)\) seconds.
The problem can be solved using the equations of motion for a particle undergoing uniformly accelerated motion. The key steps are:
Step 1: Calculate the acceleration of the particle.
The time interval is from \(t\) to \((t+1)\), so the duration is \( \Delta t = (t+1) - t = 1 \) s.
The increase in velocity during this interval is \( \Delta v = 50 \) m/s.
Assuming the acceleration is constant, it is given by:
\[ a = \frac{\Delta v}{\Delta t} = \frac{50 \, \text{m/s}}{1 \, \text{s}} = 50 \, \text{m/s}^2 \]Step 2: Calculate the velocity of the particle at time \(t\).
Let the velocity of the particle at time \(t\) be \(u\). The displacement in the time interval from \(t\) to \((t+1)\) is given as 125 m. Using the equation of motion \( s = u(\Delta t) + \frac{1}{2}a(\Delta t)^2 \):
\[ 125 = u(1) + \frac{1}{2}(50)(1)^2 \] \[ 125 = u + 25 \]Solving for \(u\):
\[ u = 125 - 25 = 100 \, \text{m/s} \]Step 3: Calculate the velocity of the particle at time \((t+1)\).
The distance travelled in the \((t+2)^{\text{th}}\) second corresponds to the displacement in the time interval from \((t+1)\) to \((t+2)\). We need the velocity at the beginning of this interval, i.e., at time \((t+1)\). Let this velocity be \(u'\).
\[ u' = u + a(\Delta t) = 100 \, \text{m/s} + (50 \, \text{m/s}^2)(1 \, \text{s}) = 150 \, \text{m/s} \]Step 4: Calculate the distance travelled in the \((t+2)^{\text{th}}\) second.
The time interval is from \((t+1)\) to \((t+2)\), so the duration is \( \Delta t = 1 \) s. The initial velocity for this interval is \( u' = 150 \) m/s.
The distance travelled (\(s'\)) in this second is:
\[ s' = u'(\Delta t) + \frac{1}{2}a(\Delta t)^2 \] \[ s' = (150)(1) + \frac{1}{2}(50)(1)^2 \] \[ s' = 150 + 25 = 175 \, \text{m} \]Since the initial velocity is positive and the acceleration is positive, the particle does not change direction, so the distance travelled is equal to the displacement.
The distance travelled by the particle in the \((t+2)^{\text{th}}\) second is 175 m.
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals:
Designate whether each of the following compounds is aromatic or not aromatic.

The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)