\( 4:1 \)
Step 1: Work done by an electric field
The work done by an electric field on a charged particle is given by: \[ W = q V \] where: - \( W \) is the work done, - \( q \) is the charge of the particle, - \( V \) is the potential difference through which the particle is accelerated.
Step 2: Charge of proton and \( \alpha \)-particle
- The charge of a proton is \( q_p = +e \). - The charge of an \( \alpha \)-particle (which is a helium nucleus) is \( q_\alpha = +2e \).
Step 3: Work done on each particle
Since both the proton and the \( \alpha \)-particle are accelerated in the same electric field, they experience the same potential difference \( V \). The work done on each is: \[ W_p = eV \] \[ W_\alpha = 2eV \]
Step 4: Work done over a given time
The kinetic energy gained by the particles is given by: \[ KE = W \] Since both particles start from rest, their velocities will be different due to their different masses, but the total work done depends only on charge and voltage. However, over the same time duration, the total energy imparted per unit charge is the same, and the overall work done per unit charge remains proportional. Thus, over a given time, the ratio of work done on the proton and the \( \alpha \)-particle remains: \[ \frac{W_p}{W_\alpha} = \frac{eV}{eV} = 1:1 \]
The magnitude of heat exchanged by a system for the given cyclic process ABC (as shown in the figure) is (in SI units):
Given the function:
\[ f(x) = \frac{2x - 3}{3x - 2} \]
and if \( f_n(x) = (f \circ f \circ \ldots \circ f)(x) \) is applied \( n \) times, find \( f_{32}(x) \).
For \( n \in \mathbb{N} \), the largest positive integer that divides \( 81^n + 20n - 1 \) is \( k \). If \( S \) is the sum of all positive divisors of \( k \), then find \( S - k \).
If the real-valued function
\[ f(x) = \sin^{-1}(x^2 - 1) - 3\log_3(3^x - 2) \]is not defined for all \( x \in (-\infty, a] \cup (b, \infty) \), then what is \( 3^a + b^2 \)?