We know that |
Surface tension (S)=$\frac{Force[F]}{Lenght[L]}$ |
So, [S] = $\frac{[MLT^{-2}]}{L}$ |
Energy (E) = Force *displacement |
[E] = [M$LT^{-2}$][L]} = [M$L^{2}T^{-2}$] |
Velocity [V] = [L$T^{-1}$] |
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Since S ∝ $E^av^bT^c$ |
where, a, b, c are constants. |
From the principle of homogeneity, |
Dimension of [LHS] = Dimension of [RHS] |
$[ML^0T^{-2}]$ = $[ML^{2}T^{-2}]^a[LT^{-1}]^b [T]^c$ |
=[$M^aL^{2a+b}T^{-2a-b+c}$] |
Equating the power on both sides, we get |
a=1 , 2a+b=0 ⇒ b=-2
-2a-b+c= -2 ⇒ c = -2
So [S] = [E$V^{-2}T^{-2}$]
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