Velocity (v) and acceleration (a) in two systems of units 1 and 2 are related as
\(v_2=\frac{n}{m^2}v_1\) and \(a_2=\frac{a_1}{mn}\)
respectively. Here m and n are constants. The relations for distance and time in two systems respectively are :
\(\frac{n^3}{m_3}L_1=L_2\) and\(\frac{n^2}{m}T_1=T_2\)
\(L_1=\frac{n^4}{m^2}L_2\) and \(T_1=\frac{n^2}{m}T_2\)
\(L_1=\frac{n^2}{m}L_2\) and \(T_1=\frac{n^4}{m^2}T_2\)
\(\frac{n^2}{m}L_1=L_2 \) and \(\frac{n^4}{m^2}T_1=T_2\)
To solve this problem, we need to understand the relationships between velocity, acceleration, distance, and time in two different systems of units. The given relationships are:
Let's use the basic kinematic equations for motion to derive the relationships for distance (\(L\)) and time (\(T\)) in these systems.
Consider the equation of motion for constant acceleration:
\(L = vt + \frac{1}{2}at^2\)
For the two systems, we have:
\(L_2 = v_2 \cdot T_2 + \frac{1}{2}a_2 \cdot T_2^2\)
Substitute the given relations \(v_2 = \frac{n}{m^2}v_1\) and \(a_2 = \frac{a_1}{mn}\) into the equation:
\(L_2 = \left(\frac{n}{m^2}v_1\right) \cdot T_2 + \frac{1}{2}\left(\frac{a_1}{mn}\right) \cdot T_2^2\)
To find the relationship between \(L_1\) and \(L_2\), note that the equation maintains homogeneity of dimensions. Thus, equating dimensions:
\(L_2 = \frac{n^3}{m^3}L_1\)
Now, consider the kinematic equations related to time (\(T\)).
Since \(v = \frac{L}{T}\) and \(a = \frac{v}{T} = \frac{L}{T^2}\), rearrange the relationships for the time:
\(T_2 = \frac{T_1 \cdot mn}{n^2}\cdot\frac{m^2}{n}\)
Simplifying, we find:
\(T_2 = \frac{n^2}{m}T_1\)
The correct relationships for distance and time between the two systems are:
Thus, the correct answer is:
\(\frac{n^3}{m^3}L_1 = L_2\) and \(\frac{n^2}{m}T_1 = T_2\).