269188
In the relation\(V=\frac{\pi p r^{4}}{8 \eta l}\) where the letters have there usual meanings the dimensions of \(\mathrm{V}\) are
1 \(M^{0} L^{3} T^{0}\)
2 \(M^{0} L^{3} T^{-1}\)
3 \(M^{0} L^{-3} T^{-1}\)
4 \(M^{1} L^{3} T^{0}\)
Explanation:
Useprinciple of homogerity
Units and Measurements
269189
If the acceleration due to gravity is\(\mathbf{1 0} \mathrm{ms}^{-2}\) and the units of length and time are changed to kilometre and hour respectively the numerical value of acceleration is
269188
In the relation\(V=\frac{\pi p r^{4}}{8 \eta l}\) where the letters have there usual meanings the dimensions of \(\mathrm{V}\) are
1 \(M^{0} L^{3} T^{0}\)
2 \(M^{0} L^{3} T^{-1}\)
3 \(M^{0} L^{-3} T^{-1}\)
4 \(M^{1} L^{3} T^{0}\)
Explanation:
Useprinciple of homogerity
Units and Measurements
269189
If the acceleration due to gravity is\(\mathbf{1 0} \mathrm{ms}^{-2}\) and the units of length and time are changed to kilometre and hour respectively the numerical value of acceleration is
269188
In the relation\(V=\frac{\pi p r^{4}}{8 \eta l}\) where the letters have there usual meanings the dimensions of \(\mathrm{V}\) are
1 \(M^{0} L^{3} T^{0}\)
2 \(M^{0} L^{3} T^{-1}\)
3 \(M^{0} L^{-3} T^{-1}\)
4 \(M^{1} L^{3} T^{0}\)
Explanation:
Useprinciple of homogerity
Units and Measurements
269189
If the acceleration due to gravity is\(\mathbf{1 0} \mathrm{ms}^{-2}\) and the units of length and time are changed to kilometre and hour respectively the numerical value of acceleration is
269188
In the relation\(V=\frac{\pi p r^{4}}{8 \eta l}\) where the letters have there usual meanings the dimensions of \(\mathrm{V}\) are
1 \(M^{0} L^{3} T^{0}\)
2 \(M^{0} L^{3} T^{-1}\)
3 \(M^{0} L^{-3} T^{-1}\)
4 \(M^{1} L^{3} T^{0}\)
Explanation:
Useprinciple of homogerity
Units and Measurements
269189
If the acceleration due to gravity is\(\mathbf{1 0} \mathrm{ms}^{-2}\) and the units of length and time are changed to kilometre and hour respectively the numerical value of acceleration is