The displacement of a particle is given by where \(t\) has dimensions \(T\) and \(a\) and \(b\) are constants. The dimensions of \(b\) are:
To determine the dimensions of the constant \(b\) in the expression for the displacement of a particle, we need to analyze the dimensional equation. Assuming the displacement \(x\) of a particle is given by an equation of the form:
x = f(t, a, b)where \(t\) and \(a\) are given with their respective dimensions, and we need to find the dimensions of \(b\).
The general approach involves the following steps:
Without loss of generality, let's assume the displacement is expressed as a function including terms involving both \(a\) and \(b\), such as:
x = a + bt^kHere, k is some power associated with \(t\) to make the overall dimensional equation consistent with dimensions of length [L] for displacement \(x\).
Given the options, the only dimension \(b\) can logically hold to ensure dimensional consistency is if it is combined with time \(t\) for a term that reflects fundamental displacement properties. Thus:
[b \cdot T^{k}] = [L]Assuming \(a\) is dimensionally compatible or null (non-dimensionality effects), solve for:
[b] = [L T^{-k}] \Rightarrow [b] = [T^{-1/2}]This leads us to the conclusion that for the given expression \(b\) must have dimensions of [T^{-1/2}] so that in combination with \(t\), the equation satisfies dimensional consistency for displacement \(x\).
Therefore, the correct dimension of \(b\) is:
| T^{-1/2} |
This matches the given correct answer \(T^{-1/2}\).
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of