1 : 4
To solve the problem, we use Wien's Displacement Law, which relates the temperature of a black body to the wavelength at which it emits the maximum energy.
The law is given by: \[ \lambda_{{max}} T = b \]
where:
- \(\lambda_{{max}}\) is the wavelength corresponding to maximum energy emission,
- \(T\) is the absolute temperature of the black body,
- \(b\) is Wien's constant (\(b \approx 2.898 \times 10^{-3} \, {m·K}\)).
Step 1: Apply Wien's Displacement Law For the two black bodies: 1. For the first black body at temperature \(T\): \[ \lambda_1 T = b \implies \lambda_1 = \frac{b}{T} \]
For the second black body at temperature \(2T\): \[ \lambda_2 (2T) = b \implies \lambda_2 = \frac{b}{2T} \]
Step 2: Find the ratio of wavelengths The ratio of the wavelengths corresponding to maximum energy emission is: \[ \frac{\lambda_1}{\lambda_2} = \frac{\frac{b}{T}}{\frac{b}{2T}} = \frac{b}{T} \cdot \frac{2T}{b} = 2 \] Thus, the ratio is: \[ \lambda_1 : \lambda_2 = 2 : 1 \]
Final Answer: The ratio between the wavelengths corresponding to maximum energy emission by the two black bodies is: \[ \boxed{2 : 1} \]
A bowl filled with very hot soup cools from $98^{\circ} C$ to $86^{\circ} C$ in 2 minutes when the room temperature is $22^{\circ} C$. How long it will take to cool from $75^{\circ} C$ to $69^{\circ} C$ ?
List I | List II | ||
A | Microwaves | i | Radioactive decay of the nucleus |
B | Gamma waves | ii | Rapid acceleration and deceleration of electrons in aerials |
C | Radio waves | iii | Inner shell electrons |
D | X - rays | iv | Klystron valve |
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: