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The potential difference (voltage) of one cell is 1,5 V. Determine the readings on V₁, V₂ and V₃ with reasons.

Physics

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Here are the solutions for the parallel circuit problems.

Part 1· 2 steps

The potential difference (voltage) of one cell is 1.5 V1.5 \text{ V}. The circuit has two cells in series, connected to three identical bulbs in parallel.

  1. Determine the total voltage supplied by the cells.

    Since there are two identical cells in series, the total voltage supplied is the sum of their individual voltages.

    Vtotal=1.5 V+1.5 V=3.0 VV_{\text{total}} = 1.5 \text{ V} + 1.5 \text{ V} = 3.0 \text{ V}

    This total voltage is measured by V3V_3, which is across the two cells. So, V3=3.0 VV_3 = 3.0 \text{ V}.

  2. Determine the voltage across the parallel bulbs.

    In a parallel circuit, the voltage across each branch (and across the entire parallel combination) is the same as the total voltage supplied by the source.

    • V1V_1 is connected across one bulb, which is a parallel branch. Therefore, V1=Vtotal=3.0 VV_1 = V_{\text{total}} = 3.0 \text{ V}.
    • V2V_2 is connected across the entire parallel combination of the three bulbs. Therefore, V2=Vtotal=3.0 VV_2 = V_{\text{total}} = 3.0 \text{ V}.

    Here is the completed table for Question 1:

    ReadingValue with unitReasonV13.0 VVoltage across parallel branches is equal to total voltage.V23.0 VVoltage across parallel combination is equal to total voltage.V33.0 VTotal voltage of 2 cells in series.\boxed{ \begin{array}{|l|l|l|} \hline \textbf{Reading} & \textbf{Value with unit} & \textbf{Reason} \\ \hline V_1 & \textbf{3.0 V} & \text{Voltage across parallel branches is equal to total voltage.} \\ \hline V_2 & \textbf{3.0 V} & \text{Voltage across parallel combination is equal to total voltage.} \\ \hline V_3 & \textbf{3.0 V} & \text{Total voltage of 2 cells in series.} \\ \hline \end{array} }

Part 2· 3 steps

In the circuit below, the resistors are identical. The reading on A2A_2 is 4 A4 \text{ A}.

  1. Determine the current through A4A_4.

    Ammeter A4A_4 is in series with the two resistors in the lower branch. In a series circuit, the current is the same at all points. Since A2A_2 measures the current in this branch, A4A_4 will have the same reading as A2A_2.

    A4=A2=4 AA_4 = A_2 = 4 \text{ A}
  2. Determine the current through A1A_1.

    Let the resistance of one resistor be RR.

    • The lower branch has two identical resistors in series, so its total resistance is Rlower=R+R=2RR_{\text{lower}} = R + R = 2R.
    • The upper branch has one resistor, so its resistance is Rupper=RR_{\text{upper}} = R.
    • In a parallel circuit, the voltage across both branches is the same. Let this voltage be VV.
    • For the lower branch: V=A2×Rlower=4 A×2R=8RV = A_2 \times R_{\text{lower}} = 4 \text{ A} \times 2R = 8R.
    • For the upper branch: V=A1×Rupper  ⟹  8R=A1×RV = A_1 \times R_{\text{upper}} \implies 8R = A_1 \times R.
    • Solving for A1A_1: A1=8RR=8 AA_1 = \frac{8R}{R} = 8 \text{ A}.
  3. Determine the current through A3A_3.

    Ammeter A3A_3 measures the total current flowing from the battery. In a parallel circuit, the total current is the sum of the currents in the individual parallel branches.

    A3=A1+A2=8 A+4 A=12 AA_3 = A_1 + A_2 = 8 \text{ A} + 4 \text{ A} = 12 \text{ A}

    Here is the completed table for Question 2:

    ReadingValue with unitReasonA18 AVoltage across parallel branches is equal. Current is inversely proportional to resistance (V/R).A24 AGivenA312 ATotal current is the sum of currents in parallel branches.A44 ACurrent is the same at all points in a series circuit (within a branch).\boxed{ \begin{array}{|l|l|l|} \hline \textbf{Reading} & \textbf{Value with unit} & \textbf{Reason} \\ \hline A_1 & \textbf{8 A} & \text{Voltage across parallel branches is equal. Current is inversely proportional to resistance (V/R).} \\ \hline A_2 & 4 \text{ A} & \text{Given} \\ \hline A_3 & \textbf{12 A} & \text{Total current is the sum of currents in parallel branches.} \\ \hline A_4 & \textbf{4 A} & \text{Current is the same at all points in a series circuit (within a branch).} \\ \hline \end{array} }
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