To find the temperature at which the resistance of the heating element is \(62 \, \Omega\), we use the formula for resistance as a function of temperature: \(R = R_0 (1 + \alpha \Delta T)\), where \(R_0\) is the initial resistance, \(\alpha\) is the temperature coefficient, and \(\Delta T\) is the change in temperature.
Given:
First, solve for \(\Delta T\):
\[\begin{align*} 62 &= 50(1 + 2.4 \times 10^{-4} \Delta T) \\ \frac{62}{50} &= 1 + 2.4 \times 10^{-4} \Delta T \\ 1.24 - 1 &= 2.4 \times 10^{-4} \Delta T \\ 0.24 &= 2.4 \times 10^{-4} \Delta T \\ \Delta T &= \frac{0.24}{2.4 \times 10^{-4}} = 1000^\circ\text{C} \end{align*}\]Next, calculate the final temperature:
\[T = T_0 + \Delta T = 27 + 1000 = 1027^\circ\text{C}\]Confirming the solution, \(1027^\circ\text{C}\) is within the expected range \(1027, 1027\). Therefore, the temperature of the element when its resistance is \(62 \, \Omega\) is \(\boxed{1027^\circ\text{C}}\).
The relationship between resistance and temperature is given by:
\[ R = R_0 \left( 1 + \alpha \Delta T \right), \]
where: \begin{itemize} \item $R_0 = 50 \, \Omega$ (resistance at room temperature), $R = 62 \, \Omega$ (resistance at the higher temperature), \(\alpha = 2.4 \times 10^{-4} \degree{C}^{-1}\) (temperature coefficient), $\Delta T = T - T_0$ (change in temperature), $T_0 = 27^\circ \mathrm{C}$ (initial temperature).
Rearrange to solve for $\Delta T$:
\[ \Delta T = \frac{R - R_0}{\alpha R_0}. \]
Substitute the given values:
\[ \Delta T = \frac{62 - 50}{(2.4 \times 10^{-4}) \cdot 50}. \]
Simplify: \[ \Delta T = \frac{12}{(2.4 \times 10^{-4}) \cdot 50} = \frac{12}{0.012} = 1000^\circ \mathrm{C}. \]
The final temperature $T$ is: \[ T = T_0 + \Delta T = 27 + 1000 = 1027^\circ \mathrm{C}. \]
A piston of mass M is hung from a massless spring whose restoring force law goes as F = -kx, where k is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature T) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $ L_0 $ to $ L_1 $, the total energy delivered by the filament is (Assume spring to be in its natural length before heating) 
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals: