To find the equilibrium separation between two molecules and their potential energy, we start by analyzing the given potential energy formula:
$$U = - \frac{A}{r^{6}} + \frac{B}{r^{12}}$$At equilibrium, the force between the molecules should be zero. The force F can be found by differentiating the potential energy with respect to the separation r:
$$F = -\frac{dU}{dr}$$Performing the differentiation:
$$\frac{dU}{dr} = \frac{d}{dr}\left(- \frac{A}{r^{6}} + \frac{B}{r^{12}}\right)$$This gives:
$$\frac{dU}{dr} = 6\frac{A}{r^{7}} - 12\frac{B}{r^{13}}$$At equilibrium, set this derivative to zero:
$$6\frac{A}{r^{7}} = 12\frac{B}{r^{13}}$$Simplifying this equation:
$$6Ar^{6} = 12B$$ $$r^{6} = \frac{2B}{A}$$Therefore, the equilibrium separation is:
$$r = \left(\frac{2B}{A}\right)^{1/6}$$Now, we substitute this equilibrium separation back into the potential energy equation to find the potential energy at equilibrium:
$$U = - \frac{A}{\left(\left(\frac{2B}{A}\right)^{1/6}\right)^{6}} + \frac{B}{\left(\left(\frac{2B}{A}\right)^{1/6}\right)^{12}}$$Simplifying each term:
$$U = - \frac{A}{\frac{2B}{A}} + \frac{B}{\frac{4B^2}{A^2}}$$ $$U = - \frac{A^2}{2B} + \frac{A^2}{4B}$$This simplifies to:
$$U = -\frac{A^2}{4B}$$Therefore, the correct answer is:
$$\left(\frac{2B}{A}\right)^{1/6}, -\frac{A^2}{4B}$$A wire of uniform resistance \(\lambda\) \(\Omega\)/m is bent into a circle of radius r and another piece of wire with length 2r is connected between points A and B (ACB) as shown in figure. The equivalent resistance between points A and B is_______ \(\Omega\).