Step 1: Expression for current in the main circuit
The total resistance in the circuit is given as the sum of the internal resistance \( r_1 \) and the effective resistance of the external circuit, which is \( \frac{3R_0}{2} \).
So, the total current in the circuit is:
\( I = \frac{E}{r_1 + \frac{3R_0}{2}} \)
Step 2: Apply Kirchhoff’s loop rule
For a loop containing the emf source and the resistors, the KVL (Kirchhoff’s Voltage Law) equation is:
\( +E - I \cdot R_0 \cdot 0.72 - I \cdot r_1 - \frac{E}{2} = 0 \)
Here,
- The potential drop across a portion of \( R_0 \) is \( I \cdot R_0 \cdot 0.72 \)
- \( I \cdot r_1 \) is the internal resistance drop
- \( \frac{E}{2} \) is a given opposing emf term
Step 3: Substitute current expression into KVL equation
Replace \( I \) with \( \frac{E}{r_1 + \frac{3R_0}{2}} \) in the KVL equation:
\( \frac{E}{2} = \frac{2E}{2r_1 + 3R_0} \cdot (0.72R_0 + r_1) \)
Step 4: Simplify the equation
Multiply both sides by 2:
\( 2r_1 + 3R_0 = 4(0.72R_0 + r_1) \)
Expand the right-hand side:
\( 2r_1 + 3R_0 = 2.88R_0 + 4r_1 \)
Step 5: Rearranging the terms
Bring like terms together:
\( 3R_0 - 2.88R_0 = 4r_1 - 2r_1 \)
\( 0.12R_0 = 2r_1 \)
Step 6: Solve for internal resistance \( r_1 \)
Divide both sides by 2:
\( r_1 = \frac{0.12R_0}{2} = 0.06R_0 \)
If \( R_0 = 50Ω \), then:
\( r_1 = 0.06 × 50 = 3Ω \)
Final Answer:
The internal resistance \( r_1 = \mathbf{3 \, \Omega} \)
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.
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
Current electricity is defined as the flow of electrons from one section of the circuit to another.
There are two types of current electricity as follows:
The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.
The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.