The potential difference between the two end terminals of an electric heater is 220 V and the current through it is 0.5 A. What would be the current through the heater if the potential difference across the terminals of the heater is reduced to 120 V?
This problem involves understanding the relationship between potential difference, current, and resistance in an electric circuit, as described by Ohm's Law. An electric heater behaves as a resistor. Assuming its resistance remains constant, we can use the initial conditions to find its resistance and then use that resistance to find the current at a different potential difference.
We are given the following information for an electric heater:
We need to find the new current, \(I_2\), through the heater when the potential difference is \(V_2\).
Ohm's Law states that the potential difference (\(V\)) across a conductor is directly proportional to the current (\(I\)) flowing through it, provided the temperature and other physical conditions remain unchanged. The constant of proportionality is the resistance (\(R\)) of the conductor. Mathematically, Ohm's Law is expressed as:
\(V = I \times R\)
From this formula, we can find the resistance using the initial values:
\(R = \frac{V_1}{I_1}\)
Let's calculate the resistance of the electric heater:
\(R = \frac{220 \text{ V}}{0.5 \text{ A}}\)
\(R = 440 \, \Omega\)
The resistance of the electric heater is \(440 \, \Omega\).
Now that we know the resistance of the heater (\(R = 440 \, \Omega\)) and the new potential difference (\(V_2 = 120\) V), we can use Ohm's Law again to find the new current (\(I_2\)).
\(V_2 = I_2 \times R\)
Rearranging the formula to solve for \(I_2\):
\(I_2 = \frac{V_2}{R}\)
Let's calculate the new current:
\(I_2 = \frac{120 \text{ V}}{440 \, \Omega}\)
\(I_2 = \frac{12}{44} \text{ A}\)
\(I_2 = \frac{3}{11} \text{ A}\)
Converting the fraction to a decimal:
\(I_2 \approx 0.2727...\) A
Rounding to two decimal places, the current is approximately 0.27 A.
| Quantity | Symbol | Formula Used | Value |
|---|---|---|---|
| Initial Potential Difference | \(V_1\) | Given | 220 V |
| Initial Current | \(I_1\) | Given | 0.5 A |
| Heater Resistance | \(R\) | \(R = V_1 / I_1\) | 440 \( \Omega \) |
| New Potential Difference | \(V_2\) | Given | 120 V |
| New Current | \(I_2\) | \(I_2 = V_2 / R\) | 0.27 A (approx) |
| Concept | Formula | Description |
|---|---|---|
| Ohm's Law | \(V = I R\) | Relates potential difference (V), current (I), and resistance (R). |
| Resistance | \(R = \frac{V}{I}\) | Resistance calculated from potential difference and current. |
| Current | \(I = \frac{V}{R}\) | Current calculated from potential difference and resistance. |
| Power | \(P = V I = I^2 R = \frac{V^2}{R}\) | Relates power (P), potential difference (V), current (I), and resistance (R). |
Electric resistance is a measure of how much a material opposes the flow of electric current. It is analogous to friction in mechanical systems. Materials with low resistance, like metals (copper, silver, aluminum), are good conductors, allowing current to flow easily. Materials with high resistance, like rubber or glass, are insulators, which restrict current flow significantly.
The resistance of a conductor depends on several factors:
The formula relating these factors is:
\(R = \frac{\rho L}{A}\)
where \(R\) is resistance, \(\rho\) is resistivity, \(L\) is length, and \(A\) is cross-sectional area. In the case of an electric heater element, the material, length, and area are fixed, so its resistance is constant under normal operating conditions, assuming temperature effects are negligible or accounted for within the context of the problem.
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