A liquid in a beaker has temperature θ(t) at time t and θ0 is temperature of surroundings, then according to Newton's law of cooling the correct graph between loge(θ – θ0) and t is :
ln(T – Ts) = ln(T0 – Ts) – kt
Newton's Law of Cooling states that the rate of cooling of a body is directly proportional to the temperature difference between the body and its surroundings. For a liquid in a beaker with temperature θ(t) at time t and θ₀ as the surrounding temperature, the law is mathematically expressed as:
where k is a positive constant. To find the relationship between ln(θ - θ₀) and time t, we can solve this differential equation.
Step 1: Separate the variables
Step 2: Integrate both sides
This gives:
where C is the constant of integration. Since θ > θ₀ during cooling, we can write:
Step 3: Interpret the equation
This is of the form y = mx + c, where y = ln(θ - θ₀), m = -k, x = t, and c = C. This represents a straight line with a negative slope (-k) and an intercept C on the ln(θ - θ₀) axis.
Therefore, the graph between ln(θ - θ₀) and time t is a straight line with a negative slope.
Final Answer: The correct graph is a straight line sloping downward, which corresponds to the second option (the image showing a decreasing linear plot).
Newton's Law of Cooling: It describes how the temperature of an object changes over time due to heat loss to its surroundings. It is applicable when the temperature difference is small, and the cooling rate is proportional to that difference.
The integrated form of Newton's Law of Cooling:
This can also be written as: , where A is a constant.