Concept:
The argument of a trigonometric function must always be dimensionless. Also, force multiplied by velocity gives power.
Step 1: Given:
\[
P=Fv\sin\beta t
\]
Since \(\sin\beta t\) is a trigonometric term, its angle \(\beta t\) must be dimensionless.
\[
[\beta t]=1
\]
\[
[\beta][t]=1
\]
\[
[\beta]=T^{-1}
\]
Step 2: Now find the dimension of \(P\).
Since \(\sin\beta t\) is dimensionless,
\[
[P]=[F][v]
\]
Dimension of force:
\[
[F]=MLT^{-2}
\]
Dimension of velocity:
\[
[v]=LT^{-1}
\]
Therefore:
\[
[P]=MLT^{-2}\times LT^{-1}
\]
\[
[P]=ML^2T^{-3}
\]
Step 3: Hence:
\[
[P]=ML^2T^{-3}, \qquad [\beta]=T^{-1}
\]
Therefore,
\[
\boxed{ML^2T^{-3},\ T^{-1}}
\]