According to Newton, the viscous force acting between liquid layers of area $A$ and velocity gradient $\Delta v/\Delta z$ is given by $F = - \eta A\frac{{\Delta v}}{{\Delta z}}$ where $\eta $ is constant called coefficient of viscosity. The dimension of $\eta $ are
According to Newton, the viscous force acting between liquid layers of area $A$ and velocity gradient $\Delta v/\Delta z$ is given by $F = - \eta A\frac{{\Delta v}}{{\Delta z}}$ where $\eta $ is constant called coefficient of viscosity. The dimension of $\eta $ are
- [AIPMT 1990]
- A
$[M{L^2}{T^{ - 2}}]$
- B
$[M{L^{ - 1}}{T^{ - 1}}]$
- C
$[M{L^{ - 2}}{T^{ - 2}}]$
- D
$[{M^0}{L^0}{T^0}]$
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