To find the temperature coefficient of resistance (\( \alpha \)) for the platinum wire, we use the formula for resistance change with temperature: \(R_t = R_0 (1 + \alpha \Delta T)\), where \(R_t\) is the resistance at temperature \( t \), \(R_0\) is the resistance at 0°C, and \(\Delta T\) is the change in temperature.
Given: \(R_0 = 2\ \Omega\), \(R_t = 6.89\ \Omega\) at \( 80°C \), \(\Delta T = 80 - 0 = 80°C\).
Substitute in the formula: \(6.89 = 2(1 + \alpha \times 80)\).
Simplifying the equation: \(6.89 = 2 + 160\alpha\).
Solve for \(\alpha\): \(6.89 - 2 = 160\alpha\), so \(4.89 = 160\alpha\).
Therefore, \(\alpha = \frac{4.89}{160}\)
Calculate: \(\alpha = 0.0305625 \degree C^{-1} \approx 3 \times 10^{-2} \degree C^{-1}\).
Thus, the temperature coefficient of resistance is \(3 \times 10^{-2} \degree C^{-1}\).
The current passing through the battery in the given circuit, is:
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second 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.