\( \left( \frac{B}{2A} \right)^{\frac{1}{5}} \)
Step 1: The equilibrium position is obtained by differentiating the potential energy function with respect to \( r \) and setting the derivative equal to zero. \[ \frac{dU}{dr} = -\frac{10A}{r^{11}} + \frac{5B}{r^6} \] Setting \( \frac{dU}{dr} = 0 \) for equilibrium: \[ -\frac{10A}{r^{11}} + \frac{5B}{r^6} = 0 \] \[ \frac{10A}{r^{11}} = \frac{5B}{r^6} \] \[ \frac{2A}{r^5} = B \] \[ r^5 = \frac{2A}{B} \] \[ r = \left( \frac{2A}{B} \right)^{\frac{1}{5}} \]
Step 2: The equilibrium distance between the atoms is \( r = \left( \frac{2A}{B} \right)^{\frac{1}{5}} \).
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
Current passing through a wire as function of time is given as $I(t)=0.02 \mathrm{t}+0.01 \mathrm{~A}$. The charge that will flow through the wire from $t=1 \mathrm{~s}$ to $\mathrm{t}=2 \mathrm{~s}$ is:
In the figure shown below, a resistance of 150.4 $ \Omega $ is connected in series to an ammeter A of resistance 240 $ \Omega $. A shunt resistance of 10 $ \Omega $ is connected in parallel with the ammeter. The reading of the ammeter is ______ mA.