To solve this problem, we need to determine the temperature \(t\) at which the resistance of a wire is \(10.95 \, \Omega\). We are given the resistance at \(0^\circ C\) is \(10 \, \Omega\) and at \(100^\circ C\) is \(10.2 \, \Omega\). The resistance \(R(t)\) of a wire at temperature \(t\) is given by: \[ R(t)=R_0(1+\alpha t) \] where \( R_0 \) is the resistance at \(0^\circ C\), \(\alpha\) is the temperature coefficient of resistance. **Step 1: Calculate \(\alpha\)** At \(100^\circ C\), we have: \[ 10.2 = 10(1 + 100\alpha) \] \[ 10.2 = 10 + 1000\alpha \] \[ 0.2 = 1000\alpha \] \[ \alpha = 0.0002 \] **Step 2: Find temperature \(t\) for resistance \(10.95 \, \Omega\)** Using the equation: \[ 10.95 = 10(1 + 0.0002t) \] \[ 10.95 = 10 + 0.002t \] \[ 0.95 = 0.002t \] \[ t = \frac{0.95}{0.002} \] \[ t = 475 \] **Step 3: Convert temperature to Kelvin scale** \[ t = 475^\circ C \] \[ T(K) = 475 + 273.15 = 748.15 \] **Step 4: Verify within range** Given the range (748, 748), \(T\) calculated as 748.15 falls within this range when rounded appropriately. Thus, the temperature \(t\) in Kelvin scale is approximately 748 K.
The temperature dependence of resistance is given by:
\[R = R_0 (1 + \alpha \Delta T).\]
From $0^\circ \text{C}$ to $100^\circ \text{C}$:
\[\frac{\Delta R}{R_0} = \alpha \Delta T \implies \alpha = \frac{10.2 - 10}{10 \cdot 100} = 0.002.\]
From $0^\circ \text{C}$ to $t^\circ \text{C}$:
\[\frac{\Delta R}{R_0} = \alpha \Delta T \implies \Delta T = \frac{10.95 - 10}{10 \cdot 0.002}.\]
\[\Delta T = 475^\circ \text{C}.\]
Convert to Kelvin:
T = 475 + 273 = 748 K
Final Answer: $748 \, \text{K}$.
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
