The work-energy theorem states that the work done on a particle is equal to the change in its kinetic energy. In this case, the retardation force is doing negative work, leading to a loss of kinetic energy.
Given \( a = -2x \), where \( a \) is acceleration and \( x \) is displacement. We can write acceleration as \( a = v \frac{dv}{dx} \), so:
\( v \frac{dv}{dx} = -2x \)
\( v \ dv = -2x \ dx \)
Integrating both sides from initial to final states:
\( \int_{v_1}^{v_2} v \ dv = -2 \int_0^x x \ dx \)
\( \frac{v_2^2}{2} - \frac{v_1^2}{2} = -x^2 \)
Multiplying by mass \( m/2 \), gives
\(KE _2 - KE_1 = \frac{1}{2}m(v_2^2 - v_1^2) = -mx^2 \)
The change in kinetic energy is \( \frac{1}{2}mv_2^2 - \frac{1}{2}mv_1^2 = -mx^2 \). Given \( m = 10 \text{ g} = 0.01 \text{ kg} = 10 \times 10^{-3} \text{ kg} = 10^{-2} \text{ kg} \).
\( \Delta KE = -mx^2 = -(10 \times 10^{-3} \text{ kg})x^2 = -10^{-2}x^2 \text{ J} \)
\( \Delta KE = -x^2 \times 10^{-2} \text{ J} \)
Comparing this with the given expression for loss of kinetic energy, \( -x^{-n} \frac{x^2 \times 10}{\frac{2}{J}} \), we find \( n = 2 \).
The value of \( n \) is \( \mathbf{2} \).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,



What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)