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The dimensional formula of a physical quantity can be obtained by defining its relation, with other quantities, whose dimensions in M, L and T are known.
Numerical Problems on Dimensional Analysis
Dimensional Formulae Practice Set
Derive dimensions and apply the principle of homogeneity(i) Angle ($\theta$):
(ii) Angular velocity ($\omega$):
(iii) Angular acceleration ($\alpha$):
(iv) Torque ($\tau$):
(v) Angular momentum ($L$):
(vi) Moment of inertia ($I$):
(i) Impulse ($J$):
(ii) Power ($P$):
(iii) Surface energy:
(iv) Coefficient of viscosity ($\eta$):
(v) Bulk modulus ($B$):
(vi) Force constant ($k$):
First, find the dimensional formula for energy per unit volume ($u$):
Next, find the dimensional formula for pressure ($P$):
Since both quantities possess the identical dimensional formula $[\text{ML}^{-1}\text{T}^{-2}]$, it is proven that energy per unit volume is dimensionally equivalent to pressure.
The dimensional formula for angular momentum ($L = mvr$) is:
Using the energy relation $E = h\nu$, we can solve for Planck’s constant $h$:
Substituting the dimensions for Energy ($[\text{ML}^2\text{T}^{-2}]$) and frequency $\nu$ ($[\text{T}^{-1}]$):
Since $[L] = [h]$, angular momentum has the same physical units as Planck’s constant (e.g., $\text{kg m}^2\text{s}^{-1}$ or $\text{J s}$).
Density ($\rho$) is defined as mass per unit volume:
We must express mass ($m$) in terms of Force ($F$), Length ($L$), and Time ($T$). From Newton’s second law, $F = m \times a$:
Substitute this back into the density formula:
Let Force $F \propto \rho^a v^b \nu^c$. Writing the standard dimensions for each:
- $[F] = [\text{MLT}^{-2}]$
- $[\rho] = [\text{ML}^{-3}\text{T}^0]$
- $[v] = [\text{M}^0\text{LT}^{-1}]$
- $[\nu] = [\text{M}^0\text{L}^0\text{T}^{-1}]$
Substitute these into the proportionality:
Equating the powers of M, L, and T:
1. For M: $a = 1$
2. For L: $-3a + b = 1 \implies -3(1) + b = 1 \implies b = 4$
3. For T: $-b – c = -2 \implies -4 – c = -2 \implies c = -2$
Therefore, the dimensional formula for Force is:
Next, for Impulse ($J$), we know $J = \text{Force} \times \text{Time}$. Since Time $t = \frac{1}{\nu} = \nu^{-1}$:
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