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A bottle of wine at room temperature \(\left(70^{\circ} \mathrm{F}\right)\) is placed in ice to chill at \(32^{\circ} \mathrm{F}\). After \(20 \mathrm{~min}\), the temperature of the wine is \(58^{\circ} \mathrm{F}\). When will its temperature be \(50^{\circ} \mathrm{F}\) ?

Short Answer

Expert verified
Approximately 33.85 minutes.

Step by step solution

01

- Understand the problem

We need to determine when the temperature of the wine reaches \(50^{\circ} \mathrm{F}\) given that it was initially \(70^{\circ} \mathrm{F}\) and in \(20 \mathrm{~min}\), it cooled to \(58^{\circ} \mathrm{F}\). The surroundings (ice) are at \(32^{\circ} \mathrm{F}\).
02

- Set up the differential equation

Newton's Law of Cooling states \[ \frac{dT}{dt} = -k(T - T_s) \] where \(T\) is the temperature of the wine, \(T_s = 32^{\circ} \mathrm{F}\) is the surrounding temperature, and \(k\) is a constant.
03

- Integrate the differential equation

Separating variables and integrating, \[ \int \frac{1}{T - T_s} dT = -k \int dt \] gives \[ \/ln|T - T_s| = -kt + C \] where \(C\) is the constant of integration.
04

- Determine the constant of integration

By using the initial condition \(T(0) = 70^{\circ} \mathrm{F}\), solve for \(C\): \[ \ln|70 - 32| = C \Rightarrow C = \ln 38. \]
05

- Solve for the constant \(k\)

Using the condition \(T(20) = 58^{\circ} \mathrm{F}\): \[ \ln|58 - 32| = -20k + \ln 38, \] solve for \(k \): \[ \ln 26 = -20k + \ln 38, \] so \[ k = \frac{\ln 38 - \ln 26}{20}. \]
06

- Set up the equation for the desired temperature

We need to find \(t\) when \(T = 50^{\circ} \mathrm{F}\): \[ \ln |50 - 32| = -kt + \ln 38. \]
07

- Solve for \(t\)

Plug in the values: \[ \ln 18 = -kt + \ln 38, \] therefore \[ t = \frac{\ln 38 - \ln 18}{k}. \]
08

- Calculate the exact value of \(t\)

Substitute the value of \(k\) from Step 5 and solve for \(t\): \[ t = \frac{\ln 38 - \ln 18}{\left(\frac{\ln 38 - \ln 26}{20}\right)} \approx 33.85 \text{ minutes}. \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Differential Equations
Differential equations play a crucial role in modeling various physical phenomena, including temperature change in Newton's Law of Cooling. Here, a differential equation describes how the temperature of an object changes over time.

Newton's Law of Cooling can be expressed as: \[ \frac{dT}{dt} = -k(T - T_s) \]
In this equation, \(T\) represents the temperature of the wine, \(T_s\) is the surrounding temperature, and \(k\) is a constant specific to the situation. The term \((T - T_s)\) indicates that the rate of temperature change depends on the difference between the object's temperature and the ambient temperature. This relationship helps us understand how the cooling process evolves over time.
Temperature Change
Understanding how temperature changes over time in Newton's Law of Cooling involves acknowledging the interaction between the object and its environment.

Initially, the wine is at room temperature \(70^{\text{°}} \text{F}\). When placed in ice at \(32^{\text{°}} \text{F}\), the wine cools to \(58^{\text{°}} \text{F}\) within 20 minutes. This temperature drop illustrates the key principle of Newton's Law — the rate of temperature change is proportional to the temperature difference.

The progression looks like this:
  • Initial temperature: \(70^{\text{°}} \text{F}\)
  • Temperature after 20 minutes: \(58^{\text{°}} \text{F}\)
  • Surrounding temperature: \(32^{\text{°}} \text{F}\)
  • Find when the wine reaches \(50^{\text{°}} \text{F}\)
    • By modeling these changes with the differential equation, we can predict the future temperature at different time intervals.
Initial Conditions
Initial conditions are critical for solving differential equations because they provide the necessary starting points. To find the specific solution to Newton's Law of Cooling, we need these initial data points.

For our wine cooling problem, the initial condition is that the wine starts at \(70^{\text{°}} \text{F}\) when \(t = 0\) minutes. Using this initial temperature helps us determine the constant of integration (\(C\)), which is essential for our final temperature function.

By substituting \(T (0) = 70\) into the integrated form, we find \[ C = \text{ln}|70 - 32| = \text{ln} 38.\]These initial conditions ensure that our model accurately reflects the specific scenario we're studying.
Integration
Integration is the process used to solve the differential equation in Newton's Law of Cooling.

First, we separate variables: \[ \frac{1}{T - T_s} dT = -k dt. \]

Next, we integrate both sides to get the natural logarithm function: \[ \text{ln}|T - T_s| = -kt + C. \] Using the initial temperature, we solve for the constant \(C\).

Finally, we use another condition — the wine temperature after 20 minutes — to find the constant \(k\). By plugging the values \(T (20) = 58\), we get: \[ k = \frac{\text{ln} 38 - \text{ln} 26}{20}. \]

Once we have \(k\), we can determine the total time needed for the wine to reach \(50^{\text{°}} \text{F}\) through additional integration and solving for \(t\). These steps show how integration helps us derive useful information from the differential equation.

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Most popular questions from this chapter

An object that weighs \(48 \mathrm{lb}\) is released from rest at the top of a plane metal slide that is inclined \(30^{\circ}\) to the horizontal. Air resistance \((\mathrm{lb})\) is numerically equal to one-half the velocity (ft/s), and the coefficient of friction is \(\mu=1 / 4\). Using Newton's second law of motion by summing the forces along the surface of the slide, we find the following forces: (a) the component of the weight parallel to the slide: \(F_{1}=48 \sin 30^{\circ}=24\); (b) the component of the weight perpendicular to the slide: \(N=48 \cos 30^{\circ}=\) \(24 \sqrt{3}\); (c) the frictional force (against the motion of the object): \(F_{2}=-\mu N=-\frac{1}{4} \times\) \(24 \sqrt{3}=-6 \sqrt{3}\); and (d) the force due to air resistance (against the motion of the object): \(F_{3}=-\frac{1}{2} v\). Because the mass of the object is \(m=\) \(48 / 32=3 / 2\), we find that the velocity of the object satisfies the initial value problem \(m d v / d t=F_{1}+F_{2}+F_{3}\) or $$ \frac{3}{2} \frac{d v}{d t}=24-6 \sqrt{3}-\frac{1}{2} v, \quad v(0)=0 . $$ Solve this problem for \(v(t)\). Determine the distance traveled by the object at time \(t\), \(x(t)\), if \(x(0)=0\).

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