To solve this problem, we must understand Ohm's Law and how it applies to the circuit described. Ohm’s Law states that the current flowing through a conductor between two points is directly proportional to the voltage across the two points, represented by the formula:
\(V = IR\)
where \(V\) is the voltage, \(I\) is the current, and \(R\) is the resistance.
If the student’s graph plots voltage as a function of current and the graph is linear going through the origin, it indicates that the system is following Ohm's Law, and there is little or no internal resistance affecting the battery.
The value of the resistance \(R\) is \(1.5 \, \Omega\):
This option gives a fixed resistance value but does not consider the internal resistance of the battery or provide information about the emf. There’s insufficient data to conclude this solely from a graph.
The emf of the battery is \(1.5 \, V\) and the value of \(R\) is \(1.5 \, \Omega\):
The emf describes the battery's voltage under no load and does not indicate resistance directly. This needs a correct analysis of both emf and resistance.
The emf of the battery is \(1.5 \, V\) and its internal resistance is \(1.5 \, \Omega\):
This option considers both emf and internal resistance, which can be validated through proper substitution in Ohm's Law and from hint \(V_0 \approx 0\).
The potential difference across the battery is \(1.5 \, V\) when it sends a current of \(1000\, mA\):
This just confirms an instance of the measured voltage at a specific current but doesn't ascertain emf or internal resistance.
Conclusion:
The correct answer is:
The emf of the battery is \(1.5\, V\) and its internal resistance is \(1.5\) \(\, \Omega\).
This option correctly identifies the emf and internal resistance based on Ohm’s Law applied to a potential difference measured across a current, assuming \(V_0 \approx 0\) signifies low or no starting value inaccuracies.