JEE PYQ: Units & Measurements - Question ID 57df0c492e35 (JEE Main 2019)

ID: 57df0c492e35JEE Main 2019Single Correct MCQ
The force of interaction between two atoms is given by F = α\alphaβ\betaexp (x2αkt)\left( { - {{{x^2}} \over {\alpha kt}}} \right); where x is the distance, k is the Boltzmann constant and T is temperature and α\alpha and β\beta are two constants. The dimension of β\beta is :

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Step-by-step Explanation

Core Formula & Concept:

In dimensional analysis, every physical quantity can be expressed in terms of the fundamental dimensions: mass (MM), length (LL), time (TT), temperature (Θ\Theta), etc. The key principle is that the dimensions on both sides of any physically meaningful equation must be identical. This is known as the principle of homogeneity of dimensions.

Given a formula involving multiple variables, we can determine the dimensions of an unknown constant by ensuring that the argument of any transcendental function (like exponential, logarithmic, or trigonometric functions) is dimensionless. Additionally, the dimensions of the entire expression must match the dimensions of the physical quantity it represents (in this case, force).

The force FF has dimensions of MLT2MLT^{-2}. The Boltzmann constant kk has dimensions of ML2T2Θ1ML^2T^{-2}\Theta^{-1}.

Step-by-Step Derivation:

The given force equation is: F=αβexp(x2αkT)F = \alpha \beta \exp \left( -\frac{x^2}{\alpha k T} \right)

  1. Analyze the exponential term: The argument of the exponential function must be dimensionless. Thus: [x2αkT]=M0L0T0\left[ \frac{x^2}{\alpha k T} \right] = M^0 L^0 T^0 Since xx is distance, [x]=L[x] = L. The Boltzmann constant kk has dimensions [k]=ML2T2Θ1[k] = ML^2T^{-2}\Theta^{-1}, and temperature TT has [Θ][\Theta]. Thus: [x2αkT]=L2[α]ML2T2Θ1Θ=L2[α]ML2T2=M0L0T0\left[ \frac{x^2}{\alpha k T} \right] = \frac{L^2}{[\alpha] \cdot ML^2T^{-2}\Theta^{-1} \cdot \Theta} = \frac{L^2}{[\alpha] \cdot ML^2T^{-2}} = M^0 L^0 T^0 Simplifying: 1[α]MT2=1    [α]=M1T2\frac{1}{[\alpha] \cdot M T^{-2}} = 1 \implies [\alpha] = M^{-1} T^2 So, the dimension of α\alpha is M1T2M^{-1}T^2.
  2. Analyze the entire force equation: The exponential term is dimensionless, so the dimensions of FF come entirely from the product αβ\alpha \beta: [F]=[α][β][F] = [\alpha] \cdot [\beta] We know [F]=MLT2[F] = MLT^{-2} and [α]=M1T2[\alpha] = M^{-1}T^2, so: MLT2=M1T2[β]MLT^{-2} = M^{-1}T^2 \cdot [\beta] Solving for [β][\beta]: [β]=MLT2M1T2=MLT2MT2=M2LT4[\beta] = \frac{MLT^{-2}}{M^{-1}T^2} = MLT^{-2} \cdot M T^{-2} = M^2 L T^{-4} Thus, the dimension of β\beta is M2LT4M^2 L T^{-4}.
Common Traps & Exam Tip:

Students often make the following mistakes in such questions:

  1. Ignoring the dimensionless nature of the exponential argument: Many students forget that the argument of the exponential function must be dimensionless, leading to incorrect dimensions for α\alpha and consequently β\beta.
  2. Miscounting dimensions of the Boltzmann constant: The Boltzmann constant kk has dimensions ML2T2Θ1ML^2T^{-2}\Theta^{-1}, not just ML2T2ML^2T^{-2}. Forgetting the temperature dimension (Θ\Theta) leads to errors.
  3. Incorrect simplification of dimensions: When solving for [β][\beta], students may incorrectly cancel or combine dimensions, especially with negative exponents. Always double-check each step.
  4. Confusing the dimensions of α\alpha and β\beta: Some students assume α\alpha is dimensionless or has the same dimensions as β\beta. Always derive dimensions systematically.

Exam Tip: Always start by ensuring the argument of any transcendental function is dimensionless. This is a powerful tool to simplify dimensional analysis problems.

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