Numerical Problems Based on Derivation of Dimensional Formulae for Class 11 Physics

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Home CBSE Class 11 Physics Numerical Problems Derivation of Dimensional Formulae

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

Class 11 Physics · Units and Measurements
SQ

Dimensional Formulae Practice Set

Derive dimensions and apply the principle of homogeneity
Ch 2 · Units and Measurements
1
Deduce dimensional formulae for (i) angle (ii) angular velocity (iii) angular acceleration (iv) torque (v) angular momentum and (vi) moment of inertia.
Answer (i) Dimensionless (ii) $[\text{T}^{-1}]$ (iii) $[\text{T}^{-2}]$ (iv) $[\text{ML}^2\text{T}^{-2}]$ (v) $[\text{ML}^2\text{T}^{-1}]$ (vi) $[\text{ML}^2]$ 📝
Detailed Solution

(i) Angle ($\theta$):

$$\text{Angle} = \frac{\text{Arc}}{\text{Radius}} = \frac{[\text{L}]}{[\text{L}]} = [\text{M}^0\text{L}^0\text{T}^0] \quad \text{(Dimensionless)}$$

(ii) Angular velocity ($\omega$):

$$\omega = \frac{\text{Angle}}{\text{Time}} = \frac{1}{[\text{T}]} = [\text{M}^0\text{L}^0\text{T}^{-1}]$$

(iii) Angular acceleration ($\alpha$):

$$\alpha = \frac{\text{Angular velocity}}{\text{Time}} = \frac{[\text{T}^{-1}]}{[\text{T}]} = [\text{M}^0\text{L}^0\text{T}^{-2}]$$

(iv) Torque ($\tau$):

$$\tau = \text{Force} \times \text{Perpendicular distance} = [\text{MLT}^{-2}] \times [\text{L}] = [\text{ML}^2\text{T}^{-2}]$$

(v) Angular momentum ($L$):

$$L = \text{Momentum} \times \text{Distance} = ([\text{M}][\text{LT}^{-1}]) \times [\text{L}] = [\text{ML}^2\text{T}^{-1}]$$

(vi) Moment of inertia ($I$):

$$I = \text{Mass} \times (\text{Distance})^2 = [\text{M}] \times [\text{L}]^2 = [\text{ML}^2\text{T}^0]$$
2
Obtain dimensions of (i) impulse (ii) power (iii) surface energy (iv) coefficient of viscosity (v) bulk modulus (vi) force constant.
Answer (i) $[\text{MLT}^{-1}]$ (ii) $[\text{ML}^2\text{T}^{-3}]$ (iii) $[\text{ML}^0\text{T}^{-2}]$ (iv) $[\text{ML}^{-1}\text{T}^{-1}]$ (v) $[\text{ML}^{-1}\text{T}^{-2}]$ (vi) $[\text{ML}^0\text{T}^{-2}]$ 📝
Detailed Solution

(i) Impulse ($J$):

$$J = \text{Force} \times \text{Time} = [\text{MLT}^{-2}] \times [\text{T}] = [\text{MLT}^{-1}]$$

(ii) Power ($P$):

$$P = \frac{\text{Work}}{\text{Time}} = \frac{[\text{ML}^2\text{T}^{-2}]}{[\text{T}]} = [\text{ML}^2\text{T}^{-3}]$$

(iii) Surface energy:

$$\text{Surface energy} = \frac{\text{Energy}}{\text{Area}} = \frac{[\text{ML}^2\text{T}^{-2}]}{[\text{L}^2]} = [\text{ML}^0\text{T}^{-2}]$$

(iv) Coefficient of viscosity ($\eta$):

$$\eta = \frac{\text{Force}}{\text{Area} \times \text{Velocity Gradient}} = \frac{[\text{MLT}^{-2}]}{[\text{L}^2] \times [\text{T}^{-1}]} = [\text{ML}^{-1}\text{T}^{-1}]$$

(v) Bulk modulus ($B$):

$$B = \frac{\text{Pressure}}{\text{Volumetric strain}} = \frac{[\text{ML}^{-1}\text{T}^{-2}]}{1} = [\text{ML}^{-1}\text{T}^{-2}]$$

(vi) Force constant ($k$):

$$k = \frac{\text{Force}}{\text{Displacement}} = \frac{[\text{MLT}^{-2}]}{[\text{L}]} = [\text{ML}^0\text{T}^{-2}]$$
3
By the use of dimensions, show that energy per unit volume is equal to the pressure.
Answer Both have dimensions $[\text{ML}^{-1}\text{T}^{-2}]$ 📝
Detailed Solution

First, find the dimensional formula for energy per unit volume ($u$):

$$u = \frac{\text{Energy}}{\text{Volume}} = \frac{[\text{ML}^2\text{T}^{-2}]}{[\text{L}^3]} = [\text{ML}^{-1}\text{T}^{-2}]$$

Next, find the dimensional formula for pressure ($P$):

$$P = \frac{\text{Force}}{\text{Area}} = \frac{[\text{MLT}^{-2}]}{[\text{L}^2]} = [\text{ML}^{-1}\text{T}^{-2}]$$

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.

4
Show that angular momentum has the same physical units as the Planck’s constant $h$ which is given by the relation $E = h\nu$.
Answer Both have dimensions $[\text{ML}^2\text{T}^{-1}]$ 📝
Detailed Solution

The dimensional formula for angular momentum ($L = mvr$) is:

$$[L] = [\text{M}] \times [\text{LT}^{-1}] \times [\text{L}] = [\text{ML}^2\text{T}^{-1}]$$

Using the energy relation $E = h\nu$, we can solve for Planck’s constant $h$:

$$h = \frac{E}{\nu}$$

Substituting the dimensions for Energy ($[\text{ML}^2\text{T}^{-2}]$) and frequency $\nu$ ($[\text{T}^{-1}]$):

$$[h] = \frac{[\text{ML}^2\text{T}^{-2}]}{[\text{T}^{-1}]} = [\text{ML}^2\text{T}^{-1}]$$

Since $[L] = [h]$, angular momentum has the same physical units as Planck’s constant (e.g., $\text{kg m}^2\text{s}^{-1}$ or $\text{J s}$).

5
If force ($F$), length ($L$) and time ($T$) are chosen as the fundamental quantities, then what would be the dimensional formula for density?
Answer $[\text{FL}^{-4}\text{T}^2]$ 📝
Detailed Solution

Density ($\rho$) is defined as mass per unit volume:

$$\rho = \frac{\text{Mass}}{\text{Volume}} = \frac{m}{L^3}$$

We must express mass ($m$) in terms of Force ($F$), Length ($L$), and Time ($T$). From Newton’s second law, $F = m \times a$:

$$m = \frac{F}{a} = \frac{F}{LT^{-2}} = [\text{FL}^{-1}\text{T}^2]$$

Substitute this back into the density formula:

$$\rho = \frac{[\text{FL}^{-1}\text{T}^2]}{[\text{L}^3]} = [\text{FL}^{-4}\text{T}^2]$$
6
Calculate the dimensions of force and impulse taking velocity ($v$), density ($\rho$) and frequency ($\nu$) as basic quantities.
Answer $[\rho v^4 \nu^{-2}]$ and $[\rho v^4 \nu^{-3}]$ 📝
Detailed Solution

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:

$$[\text{MLT}^{-2}] = [\text{ML}^{-3}]^a [\text{LT}^{-1}]^b [\text{T}^{-1}]^c$$
$$[\text{M}^1\text{L}^1\text{T}^{-2}] = [\text{M}^a \text{L}^{-3a+b} \text{T}^{-b-c}]$$

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:

$$[F] = [\rho^1 v^4 \nu^{-2}]$$

Next, for Impulse ($J$), we know $J = \text{Force} \times \text{Time}$. Since Time $t = \frac{1}{\nu} = \nu^{-1}$:

$$[J] = [F] \times [\nu^{-1}] = [\rho v^4 \nu^{-2}] \times [\nu^{-1}]$$
$$[J] = [\rho v^4 \nu^{-3}]$$

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