Numerical Problems Based on Deriving Relationship between Physical Quantities for Class 11 Physics

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Home CBSE Class 11 Physics Numerical Problems Numerical Problems Based on Deriving Relationship between Physical Quantities for Class 11 Physics

By using the principle of homogeneity of dimen­sions, the form of expression for a given physical quantity can be obtained if we know the factors upon which that physical quantity depends.

Numerical Problems on Dimensional Analysis

Class 11 Physics · Units and Measurements
SQ

Derivation of Formulae Practice Set

Apply the method of dimensions to deduce physical relations
Ch 2 · Units and Measurements
1
The wavelength $\lambda$ associated with a moving electron depends on its mass $m$, its velocity $v$ and Planck’s constant $h$. Prove dimensionally that $\lambda \propto \frac{h}{mv}$. [Himachal 04 ; Chandigarh 08]
Answer Proof completed 📝
Detailed Solution

(Note: The original prompt had a typo “$\lambda \propto \frac{\lambda}{mv}$”, corrected here to $\frac{h}{mv}$).

Let the relation be $\lambda \propto m^a v^b h^c$, which can be written as $\lambda = K m^a v^b h^c$, where $K$ is a dimensionless constant.

Writing the dimensions of each quantity:

  • $[\lambda] = [\text{L}]$
  • $[m] = [\text{M}]$
  • $[v] = [\text{LT}^{-1}]$
  • $[h] = [\text{ML}^2\text{T}^{-1}]$

Substitute these into the equation:

$$[\text{L}] = [\text{M}]^a [\text{LT}^{-1}]^b [\text{ML}^2\text{T}^{-1}]^c$$
$$[\text{M}^0\text{L}^1\text{T}^0] = [\text{M}^{a+c}\text{L}^{b+2c}\text{T}^{-b-c}]$$

Applying the Principle of Homogeneity, equate the powers of M, L, and T:

1. For M: $a + c = 0 \implies a = -c$
2. For T: $-b – c = 0 \implies b = -c$
3. For L: $b + 2c = 1$

Substitute $b = -c$ into equation (3):

$$-c + 2c = 1 \implies c = 1$$

Since $c = 1$, we get $a = -1$ and $b = -1$.

Substituting the values of $a, b, c$ back into the original relation:

$$\lambda = K m^{-1} v^{-1} h^1 = K \frac{h}{mv}$$

Therefore, $\lambda \propto \frac{h}{mv}$.

2
Obtain an expression for the centripetal force $F$ acting on a particle of mass $m$ moving with velocity $v$ in a circle of radius $r$. Take dimensionless constant $K=1$. [Himachal 2000]
Answer $F = \frac{mv^2}{r}$ 📝
Detailed Solution

Let the force depend on mass $m$, velocity $v$, and radius $r$ as follows: $F = K m^a v^b r^c$.

Writing the dimensions of each physical quantity:

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

Equating the powers of M, L, and T:

1. For M: $a = 1$
2. For T: $-b = -2 \implies b = 2$
3. For L: $b + c = 1 \implies 2 + c = 1 \implies c = -1$

Substituting $a, b, c$ into the formula:

$$F = K m^1 v^2 r^{-1} = K \frac{mv^2}{r}$$

Since it is given that $K = 1$, the final expression is:

$$F = \frac{mv^2}{r}$$
3
The orbital velocity $v$ of a satellite may depend on its mass $m$, the distance $r$ from the centre of the earth and acceleration due to gravity $g$. Obtain an expression for its orbital velocity.
Answer $v = K\sqrt{rg}$ 📝
Detailed Solution

Let $v = K m^a r^b g^c$.

Writing the dimensions of the respective quantities:

$$[\text{LT}^{-1}] = [\text{M}]^a [\text{L}]^b [\text{LT}^{-2}]^c$$
$$[\text{M}^0\text{L}^1\text{T}^{-1}] = [\text{M}^a \text{L}^{b+c} \text{T}^{-2c}]$$

Equating the powers of M, L, and T:

1. For M: $a = 0$ (This shows velocity is independent of mass $m$).
2. For T: $-2c = -1 \implies c = \frac{1}{2}$
3. For L: $b + c = 1 \implies b + \frac{1}{2} = 1 \implies b = \frac{1}{2}$

Substituting the values of $a, b,$ and $c$ into the assumed relation:

$$v = K m^0 r^{1/2} g^{1/2} = K(rg)^{1/2}$$
$$v = K\sqrt{rg}$$
4
A small spherical ball of radius $r$ falls with velocity $v$ through a liquid having coefficient of viscosity $\eta$. Find the viscous drag $F$ on the ball assuming it depends on $\eta, r$ and $v$. Take $K=6\pi$.
Answer $F = 6\pi\eta rv$ 📝
Detailed Solution

Let the viscous force $F$ be expressed as $F = K \eta^a r^b v^c$.

Writing dimensions on both sides:

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

Equating the corresponding powers of M, L, and T:

1. For M: $a = 1$
2. For T: $-a – c = -2 \implies -1 – c = -2 \implies c = 1$
3. For L: $-a + b + c = 1 \implies -1 + b + 1 = 1 \implies b = 1$

Substituting $a=1, b=1, c=1$ back into the equation:

$$F = K \eta^1 r^1 v^1 = K\eta rv$$

Given $K = 6\pi$, we get Stokes’ Law:

$$F = 6\pi\eta rv$$
5
The velocity of a freely falling body is a function of the distance fallen through ($h$) and acceleration due to gravity $g$. Show by the method of dimensions that $v = K\sqrt{gh}$.
Answer Proof completed 📝
Detailed Solution

Let the velocity $v$ depend on height $h$ and gravity $g$ as follows: $v = K h^a g^b$.

Writing the dimensional formulas on both sides:

$$[\text{LT}^{-1}] = [\text{L}]^a [\text{LT}^{-2}]^b$$
$$[\text{L}^1\text{T}^{-1}] = [\text{L}^{a+b} \text{T}^{-2b}]$$

Equating the powers of L and T:

1. For T: $-2b = -1 \implies b = \frac{1}{2}$
2. For L: $a + b = 1 \implies a + \frac{1}{2} = 1 \implies a = \frac{1}{2}$

Substituting $a$ and $b$ back into the original relation:

$$v = K h^{1/2} g^{1/2} = K(gh)^{1/2}$$
$$v = K\sqrt{gh}$$

Hence proved.

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