To solve the problem, we need to find the heat required to raise the temperature of 1 kg of a substance from $-73^{\circ}C$ to $27^{\circ}C$.
1. Understanding the Specific Heat Capacity Relation:
The specific heat capacity of the substance is given by $C = kT$, where $k$ is a constant and $T$ is the absolute temperature.
2. Converting Temperatures to Kelvin:
We have $T_1 = -73^{\circ}C = -73 + 273 = 200 \, \text{K}$ and $T_2 = 27^{\circ}C = 27 + 273 = 300 \, \text{K}$.
3. Formula for Heat Required:
The heat required is given by:
$ Q = \int_{T_1}^{T_2} mC \, dT = \int_{T_1}^{T_2} m(kT) \, dT$
where $m = 1$ kg.
4. Simplifying the Integral:
We now have:
$ Q = \int_{200}^{300} 1(kT) \, dT = k \int_{200}^{300} T \, dT = k \left[ \frac{T^2}{2} \right]_{200}^{300}$
5. Calculating the Integral:
This becomes:
$ Q = k \left(\frac{300^2}{2} - \frac{200^2}{2} \right) = k \left(\frac{90000}{2} - \frac{40000}{2} \right)$
6. Final Simplification:
We get:
$ Q = k \left(\frac{50000}{2} \right) = k (25000)$
7. Solving for $n$:
Given that $Q = nk$, we have:
$ nk = 25000k$
This implies:
$ n = 25000$
Final Answer:
The final answer is $\boxed{25000}$.
To solve the problem, we calculate the heat required to raise the temperature of 1 kg of the substance when its specific heat capacity depends on temperature.
Given:
Specific heat capacity:
\[
C = k T
\]
where \(k\) is a constant and \(T\) is the absolute temperature (in Kelvin).
Temperature change from \(-73^\circ C\) to \(27^\circ C\).
Step 1: Convert temperatures to Kelvin:
\[
T_1 = -73 + 273 = 200\, K
\]
\[
T_2 = 27 + 273 = 300\, K
\]
Step 2: Calculate heat required:
Heat for mass \(m = 1\, kg\) with variable heat capacity:
\[
Q = m \int_{T_1}^{T_2} C \, dT = \int_{200}^{300} k T \, dT = k \int_{200}^{300} T \, dT
\]
\[
Q = k \left[ \frac{T^2}{2} \right]_{200}^{300} = k \left( \frac{300^2}{2} - \frac{200^2}{2} \right) = \frac{k}{2} (90000 - 40000) = \frac{k}{2} \times 50000 = 25000 k
\]
Step 3: Express heat as \(n k\):
\[
Q = n k \implies n = 25000
\]
Final Answer:
\[
\boxed{25000}
\]
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):