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JEE Main 20137 April
Exam
JEE Main
Year
2013
Date
7 April
Subject
Physics
Chapter
Thermal Properties of Matter

JEE Main 2013 · 7 April · Physics · Thermal Properties of Matter

If a piece of metal is heated to temperature θ and then allowed to...

If a piece of metal is heated to temperatureθ\theta and then allowed to cool in a room which is at temperatureθ0{\theta}_{0}, the graph between the temperature TT of the metal and time tt will be closest to :If a piece of metal is heated to temperature θ and then allowed to cool in a room which is at temperature θ _ 0 , theIf a piece of metal is heated to temperature θ and then allowed to cool in a room which is at temperature θ _ 0 , theIf a piece of metal is heated to temperature θ and then allowed to cool in a room which is at temperature θ _ 0 , theIf a piece of metal is heated to temperature θ and then allowed to cool in a room which is at temperature θ _ 0 , the

Options

  1. AWavelength of light used in an optical instrument are λ_1=4000 Å and λ_2=5000 Å , then ratio of their respective
  2. BWavelength of light used in an optical instrument are λ_1=4000 Å and λ_2=5000 Å , then ratio of their respective
  3. CWavelength of light used in an optical instrument are λ_1=4000 Å and λ_2=5000 Å , then ratio of their respective
  4. DWavelength of light used in an optical instrument are λ_1=4000 Å and λ_2=5000 Å , then ratio of their respective

Correct answer

A. Wavelength of light used in an optical instrument are λ_1=4000 Å and λ_2=5000 Å , then ratio of their respective

Step-by-step solution

According to Newton's cooling law, rate of cooling is

dθdt∝(θ−θ0)\dfrac{d \theta}{d t} ∝ \left(\theta - {\theta}_{0}\right)

Here, θ=\theta =the temperature of the body

θ0={\theta}_{0} =Room temperature(constant)

Let kk be the proportionality constant and θi{\theta}_{i} be the initial temperature.
Therefore,

dθdt=−k(θ−θ0)⇒∫dθ(θ−θ0)=−k∫dt⇒ln⁡(θ−θ0)=−kt⇒θ=θ0+(θ−θ0)e−kt\dfrac{d \theta}{d t} = - k\left(\theta - {\theta}_{0}\right) ⇒ ∫ \dfrac{d \theta}{\left(\theta - {\theta}_{0}\right)} = - k ∫ d t ⇒ \ln \left(\theta - {\theta}_{0}\right) = - kt ⇒ \theta = {\theta}_{0} + \left(\theta - {\theta}_{0}\right){e}^{- kt}

Hence, the graph is exponential.

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