The problem provides the following values:
The terminal voltage ($V_T$) of a battery is the actual voltage across its terminals when current is flowing. It can be calculated using the formula:
$ V_T = \mathcal{E} - Ir $
Where:
Substitute the given values into the formula:
$ V_T = 12 \text{ V} - (0.6 \text{ A} \times 2 \ \Omega) $
First, calculate the voltage drop across the internal resistance:
$ I \times r = 0.6 \text{ A} \times 2 \ \Omega = 1.2 \text{ V} $
Now, subtract this voltage drop from the battery's emf:
$ V_T = 12 \text{ V} - 1.2 \text{ V} $
$ V_T = 10.8 \text{ V} $
The terminal voltage of the battery is $10.8 \text{ V}$.
In the circuit shown below, the voltage appearing across the diode D will be of the form :
A 100-turn closely wound circular coil of radius $10 \text{ cm}$ has a magnetic field of $3.14 \times 10^{-3} \text{ T}$ at its centre. The current passing through the coil, and the magnitude of the magnetic moment of this coil are, respectively :
(Take $\mu_0 = 4\pi \times 10^{-7} \text{ T m/A}$)
The current $I$ in the circuit shown below is :
(All diodes are ideal and identical.

The figure given below shows a long straight solid wire of circular cross-section of radius 'a' carrying steady current I. The current I is uniformly distributed across its cross-section. The plot which correctly represents the variation of magnetic field (B) with distance (r) from the axis of the conductor in the region is :
Five capacitors of capacitances $C_1 = C_2 = C_3 = C_4 = 10 \ \mu\text{F}$ and $C_5 = 2.5 \ \mu\text{F}$ are connected as shown along with a battery of $50 \text{ V}$. 
The equivalent capacitance and the charges on each capacitor respectively are :
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by $15 \text{ cm}$ length of wire $Q$ is________.
$(\mu_o = 4\pi \times 10^{-7} \text{ T.m/A})$