Step 1: Identify the dimensional nature of the sine argument.
In the wave equation \(y = a\sin(bt - cx)\), the quantity inside sine must be dimensionless.
So,
\[
bt - cx \;\; \text{must be dimensionless}
\]
Step 2: Check dimensions of each term.
Since \(bt\) is dimensionless,
\[
[b][t] = 1 \Rightarrow [b] = T^{-1}
\]
Similarly, \(cx\) is dimensionless,
\[
[c][x] = 1 \Rightarrow [c] = L^{-1}
\]
Step 3: Test each option.
(A) \(\dfrac{y}{a}\): Since \(y\) has same dimension as \(a\), ratio is dimensionless.
(B) \(bt\): Dimensionless as proved above.
(C) \(cx\): Dimensionless as proved above.
(D) \(\dfrac{b}{c}\):
\[
\left[\frac{b}{c}\right] = \frac{T^{-1}}{L^{-1}} = LT^{-1}
\]
This has dimensions of velocity, so it is a dimensional quantity.
Final Answer:
\[
\boxed{\dfrac{b}{c}}
\]