The image illustrates an electrical circuit containing two voltage sources and three resistors, connected in parallel and series combinations. The components are labeled as follows:1. **Voltage Sources:** - \(\xi_1\) - \(\xi_2\)2. **Resistors:** - \(R_1\), connected in series with \(\xi_1\) - \(R_2\), connected in series with \(\xi_2\) - \(R_3\), connects the ends of the circuit in parallel to both \(R_1\) and \(R_2\)3. **Currents:** - \(I_1\), flows through \(R_1\) - \(I_2\), flows through \(R_2\) - \(I_3\), flows through \(R_3\)**Explanation:**- The circuit consists of a closed loop with two branches formed by the two sets of a voltage source and a resistor (\(\xi_1, R_1\) and \(\xi_2, R_2\)).- In the parallel section, \(R_3\) is connected between the two branches, and current \(I_3\) flows through it from right to left.- The flow of currents is as follows: - \(I_1\) flows from left to right through the resistor \(R_1\). - \(I_2\) flows from right to left through the resistor \(R_2\). - \(I_3\) flows through \(R_3\) in the horizontal section of the circuit, indicated with the arrow pointing left.This circuit could be analyzed to find the relationships between the given currents and voltages using Kirchhoff's laws or other circuit analysis techniques. **Title: Kirchhoff's Voltage Law: Deriving Equations for Circuit Loops****Objective:**To apply Kirchhoff’s Voltage Law (KVL) in deriving two distinct equations that describe the potential differences across components within two separate complete loops of a given circuit.**Instructions:**1. **Understanding the Task:** - Utilize Kirchhoff’s Voltage Law with the provided variables. - Formulate equations for the potential differences across the components in two complete loops.2. **Variables:** - \( \xi_1, \xi_2 \): Electromotive forces (emfs) in the circuit. - \( R_1, R_2, R_3 \): Resistances within the circuit. - \( I_1, I_2 \): Currents flowing through different paths.3. **Kirchhoff’s Voltage Law Recap:** - Kirchhoff’s Voltage Law states that the sum of the potential differences (voltage) around any closed loop in a circuit must equal zero. \[ \sum_{i=1}^{n} \Delta V_i = 0 \] where \( \Delta V_i \) represents the potential difference across the \( i \)-th component in the loop.**Guidance for Writing Equations:**Consider setting up two individual loop equations, ensuring that the sum of all voltage contributions (both supplies and drops) within each loop equals zero—this includes accounting for resistors and emfs through each loop. Use the symbols (\( \xi_1, \xi_2, R_1, R_2, R_3, I_1, I_2 \)) to express these relationships mathematically based on their arrangement in the circuit.**Note:** Carefully observe the direction of currents and potential differences as influenced by the direction assumed in each loop during calculations.

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a) Use Kirchhoff's Voltage Law and the given variables to write down two unique equations involving the potential differences across the components in two different complete loops. Your answers should be in terms of či, č2, R1, R2, R3, I1, and I2, as needed. Recall that Kirchhoff's Voltage Law for the potential difference across the components of a circuit in a complete loop is given as >'av = 0 where AV, is the potential difference across the ith component in the loop.

a) Use Kirchhoff's Voltage Law and the given variables to write down two unique equations involving the potential differences across the components in two different complete loops. Your answers should be in terms of či, č2, R1, R2, R3, I1, and I2, as needed. Recall that Kirchhoff's Voltage Law for the potential difference across the components of a circuit in a complete loop is given as >'av = 0 where AV, is the potential difference across the ith component in the loop.