To construct a dimensionless quantity from \( e \), \(\epsilon_0\), \( h \), and \( c \), we assign their respective dimensional formulas with powers \(\alpha\), \(\beta\), \(\gamma\), and \(\delta\). The expression takes the form:
\( e^\alpha \epsilon_0^\beta h^\gamma c^\delta \)
The dimensions of each quantity are:
The dimensionless condition implies:
\([M]^0[L]^0[T]^0[I]^0\) for the product \( e^\alpha \epsilon_0^\beta h^\gamma c^\delta \)
Equating powers for each dimension:
1. Mass (M):
\(0 = \beta(-1) + \gamma(1) = -\beta + \gamma\) (Equation 1)
2. Length (L):
\(0 = \beta(-3) + \gamma(2) + \delta(1) = -3\beta + 2\gamma + \delta\) (Equation 2)
3. Time (T):
\(0 = \beta(4) + \gamma(-1) + \delta(-1) + \alpha(1) = 4\beta - \gamma - \delta + \alpha\) (Equation 3)
4. Current (I):
\(0 = \alpha(1) + \beta(2) = \alpha + 2\beta\) (Equation 4)
By solving these equations systematically:
From Equation 4: \(\alpha = -2\beta\)
Substitute \(\alpha = -2\beta\) into Equation 3:
\(4\beta - \gamma - \delta - 2\beta = 0\)
\(2\beta - \gamma - \delta = 0\) (Equation 5)
Use Equation 1:\( -\beta + \gamma = 0 \ => \ \gamma = \beta\)
Substitute \(\gamma = \beta\) in Equation 5:
\(2\beta - \beta - \delta = 0\)
\(\beta = \delta\)
Hence, \(\alpha = -2\beta = -2\delta\)
Thus, \(\alpha = 2n\), \(\beta = -n\), \(\gamma = -n\), \(\delta = -n\), as \(n\) is a non-zero integer.
The tuple \((\alpha, \beta, \gamma, \delta)\) is \((2n, -n, -n, -n)\).
Let's verify the correct set of exponents \((\alpha, \beta, \gamma, \delta)\) so that
\[ e^\alpha \epsilon_0^\beta h^\gamma c^\delta \] is dimensionless. ---
Step 1: Dimensions of each quantity
- Charge \(e\): \([I T]\) - Permittivity \(\epsilon_0\): \([M^{-1} L^{-3} T^4 I^2]\) - Planck's constant \(h\): \([M L^2 T^{-1}]\) - Speed of light \(c\): \([L T^{-1}]\) ---
Step 2: Express combined dimension
\[ [I]^{\alpha + 2 \beta} \cdot [M]^{-\beta + \gamma} \cdot [L]^{-3 \beta + 2 \gamma + \delta} \cdot [T]^{\alpha + 4 \beta - \gamma - \delta} \] ---
Step 3: Set exponents to zero
\[ \begin{cases} \alpha + 2 \beta = 0 \\ -\beta + \gamma = 0 \\ -3 \beta + 2 \gamma + \delta = 0 \\ \alpha + 4 \beta - \gamma - \delta = 0 \end{cases} \] ---
Step 4: Solve the system
From second: \(\gamma = \beta\) From first: \(\alpha = -2 \beta\) Substitute in third: \[ -3 \beta + 2 \beta + \delta = 0 \implies -\beta + \delta = 0 \implies \delta = \beta \] Substitute in fourth: \[ -2 \beta + 4 \beta - \beta - \beta = 0 \implies 0=0 \] All consistent. ---
Step 5: Express in terms of \(n = \beta\)
\[ (\alpha, \beta, \gamma, \delta) = (-2n, n, n, n) \] ---
Step 6: Compare with given options
Given options are multiples of \(n\), so multiply both sides by \(-1\) (valid since \(n\) is any non-zero integer): \[ (2n, -n, -n, -n) \] This matches the first option. ---
Final answer:
\[ \boxed{ (2n, -n, -n, -n) } \]
The graph shows the variation of current with voltage for a p-n junction diode. Estimate the dynamic resistance of the diode at \( V = -0.6 \) V.

Assertion (A): We cannot form a p-n junction diode by taking a slab of a p-type semiconductor and physically joining it to another slab of an n-type semiconductor.
Reason (R): In a p-type semiconductor, \( n_e \gg n_h \) while in an n-type semiconductor \( n_h \gg n_e \).
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is: