Dimensional analysis is a powerful tool. When expressing a quantity in terms of new fundamental quantities, use the dimensional formulas of all quantities and equate the exponents of each fundamental dimension.
Let \( M \) be the mass, and let its dimensions in terms of \( h \), \( c \), and \( G \) be given by:
\[ M = h^x c^y G^z \]
The dimensions of \( h \) (Planck’s constant) are \([ML^2T^{-1}]\). The dimensions of \( c \) (speed of light) are \([LT^{-1}]\). The dimensions of \( G \) (gravitational constant) are \([M^{-1}L^3T^{-2}]\). Substituting these dimensions into the equation from Step 1, we get:
\[ [M] = [M L^2 T^{-1}]^x [L T^{-1}]^y [M^{-1} L^3 T^{-2}]^z \]
\[ [M^1 L^0 T^0] = [M^x L^{2x} T^{-x}] [L^y T^{-y}] [M^{-z} L^{3z} T^{-2z}] \]
\[ [M^1 L^0 T^0] = [M^{x-z} L^{2x+y+3z} T^{-x-y-2z}] \]
Equating the exponents of \( M \), \( L \), and \( T \) on both sides, we get the following system of equations:
Adding the second and third equations, we get:
\[ x + z = 0 \]
Also, from the first equation, \( x - z = 1 \). Adding these two equations gives \( 2x = 1 \), so \( x = \frac{1}{2} \). Since \( x + z = 0 \), we have \( z = -\frac{1}{2} \). Substituting \( x \) and \( z \) into the third equation gives:
\[ -\frac{1}{2} - y - 2\left(-\frac{1}{2}\right) = 0 \]
\[ -\frac{1}{2} - y + 1 = 0 \]
\[ y = \frac{1}{2} \]
Thus, \( x = \frac{1}{2} \), \( y = \frac{1}{2} \), and \( z = -\frac{1}{2} \).
Therefore, the dimensions of mass in the new system are:
\[ M = h^{\frac{1}{2}} c^{\frac{1}{2}} G^{-\frac{1}{2}} \]
The correct answer is option (3).
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ is:
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of:
Let one focus of the hyperbola $ \frac{x^2}{a^2} - \frac{y^2}{b^2} = 1 $ be at $ (\sqrt{10}, 0) $, and the corresponding directrix be $ x = \frac{\sqrt{10}}{2} $. If $ e $ and $ l $ are the eccentricity and the latus rectum respectively, then $ 9(e^2 + l) $ is equal to:
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
A unit of a physical quantity is an arbitrarily chosen standard that is broadly acknowledged by the society and in terms of which other quantities of similar nature may be measured.
The process of measurement is basically a comparison process. To measure a physical quantity, we have to find out how many times a standard amount of that physical quantity is present in the quantity being measured. The number thus obtained is known as the magnitude and the standard chosen is called the unit of the physical quantity.
Read More: Fundamental and Derived Units of Measurement
The units defined for the fundamental quantities are called fundamental units.
The units of all other physical quantities which are derived from the fundamental units are called the derived units.