To determine the correct exponents πΌ, π½, and πΎ for expressing Youngβs modulus of elasticity, π, in terms of the gravitational constant πΊ, Planckβs constant β, and the speed of light π, we must equate the dimensions on both sides of the equation: π = ππΌβπ½πΊπΎ. The dimension of Youngβs modulus π is [ML-1T-2].
Let's consider the dimensions of each of the constants:
The equation becomes: [ML-1T-2] = [LT-1]πΌ[ML2T-1]π½[M-1L3T-2]πΎ.
Equating dimensions on both sides:
Solving these equations:
This provides the correct exponents: Ξ± = 7, Ξ² = -1, Ξ³ = -2, confirming the correct Option:
πΌ = 7, π½ = β1, πΎ = β2.
The given equation is:
\(Y = c^\alpha h^\beta G^\gamma\)
We are also given the following dimensional relations:
\([M L^{-1} T^{-2}] = [M^0 L^1 T^{-1}]^\alpha [M L^2 T^{-1}]^\beta [M^{-1} L^3 T^{-2}]^\gamma\)
Equating the powers of \( M \), \( L \), and \( T \), we get the following system of equations:
\(1 = \beta - \gamma\)
\(-1 = \alpha + 2\beta + 3\gamma\)
\(-2 = -\alpha - \beta - 2\gamma\)
Now, solving this system of equations:
From the first equation: \( \beta = 1 + \gamma \)
Substitute this into the second and third equations:
\(-1 = \alpha + 2(1 + \gamma) + 3\gamma\)
\(-2 = -\alpha - (1 + \gamma) - 2\gamma\)
Solving these equations results in:
\(\alpha = 7, \quad \beta = -1, \quad \gamma = -2\)
Thus, the correct option is (A): \( \alpha = 7 \), \( \beta = -1 \), \( \gamma = -2 \).
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
Read More: Youngβs Double Slit Experiment