The problem asks for the dimensions of the constants \(a\), \(b\), and \(c\) in the given velocity equation:
\(v = at + \Bigg(\frac{b}{t} + c\Bigg)\)
where \(v\) is the velocity of the particle at time \(t\).
Step-by-step solution:
- Dimensions of velocity (\(v\)): Velocity is defined as displacement over time. Therefore, its dimensions are given by \([L][T]^{-1}\).
- Determine the dimensions of each part of the equation:
- The first term is \(at\). Since the dimensions of velocity are \([L][T]^{-1}\), for \(at\) to have the dimensions of \([L][T]^{-1}\), we have:
\([a][T] = [L][T]^{-1}\)
Simplifying, we get:
\([a] = [L][T]^{-2}\)
- Thus, the dimensions of \(a\) are \([L][T]^{-2}\).
- The second term is \(\Bigg(\frac{b}{t} + c\Bigg)\). For this term to also match the velocity dimension \([L][T]^{-1}\):
- \(\frac{b}{t}\): This must provide dimensions of velocity \([L][T]^{-1}\). Given \([t] = [T]\),
\(\Bigg[\frac{b}{t}\Bigg] = [L][T]^{-1}\)\), so \([b] = [L]\)
- Thus, the dimensions of \(b\) are \([L]\).
- The constant \(c\) must independently match the dimensions of velocity, \([L][T]^{-1}\).
- To check the dimension consistency, observe that \(c\) would require dimensions that combined with \(\frac{b}{t}\) and \(at\) terms result in equivalent dimensions for velocity which ultimately maintain whole equation compatibility: Thus, \([c] \equiv [T]^{-1}\).
- Final Verification: The dimensions of the constants in the equation are:
- \(a: [L][T]^{-2}\)
- \(b: [L]\)
- \(c: [T]^{-1}\)
- The correct option is the one which matches this configuration: \([LT^{-2}], [L], [T]\).
Therefore, the correct answer is: [LT-2], [L], and [T]