College Algebra

Newton's Law of Cooling

Last updated: March 2026 · Advanced
Real-world applications
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HVAC

Refrigerant charging, airflow, system sizing

πŸ’Š
Nursing

Medication dosages, IV drip rates, vital monitoring

When you take a hot cup of coffee and set it on a table, it cools down. But it does not cool at a constant rate β€” it cools faster at first (when the temperature difference from the room is large) and slower later (when it is closer to room temperature). This behavior is captured precisely by Newton’s Law of Cooling, one of the most elegant applications of exponential functions.

The Model

Newton’s Law of Cooling states that the temperature of an object changes at a rate proportional to the difference between its temperature and the surrounding (ambient) temperature. The resulting formula is:

T(t)=Ts+(T0βˆ’Ts)eβˆ’ktT(t) = T_s + (T_0 - T_s)e^{-kt}

where:

  • T(t)T(t) = temperature of the object at time tt
  • TsT_s = surrounding (ambient) temperature
  • T0T_0 = initial temperature of the object (at t=0t = 0)
  • kk = cooling constant (k>0k > 0)
  • tt = time

Understanding the Formula

At t=0t = 0: T(0)=Ts+(T0βˆ’Ts)e0=Ts+T0βˆ’Ts=T0T(0) = T_s + (T_0 - T_s)e^0 = T_s + T_0 - T_s = T_0 β€” the initial temperature.

As tβ†’βˆžt \to \infty: eβˆ’ktβ†’0e^{-kt} \to 0, so Tβ†’TsT \to T_s β€” the object approaches room temperature.

The term (T0βˆ’Ts)eβˆ’kt(T_0 - T_s)e^{-kt} represents the temperature excess (or deficit) above (or below) the ambient temperature, and it decays exponentially.

Cooling: When T0>TsT_0 > T_s (object hotter than surroundings), the temperature decreases toward TsT_s.

Warming: When T0<TsT_0 < T_s (object cooler than surroundings), the formula still works β€” the temperature increases toward TsT_s. For example, a cold drink warming up in a hot room.

Finding the Cooling Constant kk

The constant kk depends on the physical properties of the object and its environment (material, surface area, air circulation). You find kk from a data point: if you know the temperature at some specific time, you can solve for kk.

Example 1: A cup of coffee is brewed at 200 degrees F and placed in a 72-degree room. After 5 minutes, the coffee is 180 degrees. Find kk and the complete model.

Given: T0=200T_0 = 200, Ts=72T_s = 72, T(5)=180T(5) = 180.

Setup:

180=72+(200βˆ’72)eβˆ’5k180 = 72 + (200 - 72)e^{-5k}

180=72+128eβˆ’5k180 = 72 + 128e^{-5k}

108=128eβˆ’5k108 = 128e^{-5k}

eβˆ’5k=108128=0.84375e^{-5k} = \frac{108}{128} = 0.84375

βˆ’5k=ln⁑(0.84375)=βˆ’0.16990-5k = \ln(0.84375) = -0.16990

k=0.03398k = 0.03398

Model: T(t)=72+128eβˆ’0.03398tT(t) = 72 + 128e^{-0.03398t}

Verification: T(5)=72+128eβˆ’0.170=72+128Γ—0.8438=72+108=180T(5) = 72 + 128e^{-0.170} = 72 + 128 \times 0.8438 = 72 + 108 = 180 degrees F. Confirmed.

Solving for Time

Once you have the model, you can solve for when the object reaches a specific temperature.

Example 2 (Continuing from Example 1): When will the coffee cool to 120 degrees?

120=72+128eβˆ’0.03398t120 = 72 + 128e^{-0.03398t}

48=128eβˆ’0.03398t48 = 128e^{-0.03398t}

eβˆ’0.03398t=0.375e^{-0.03398t} = 0.375

βˆ’0.03398t=ln⁑(0.375)=βˆ’0.9808-0.03398t = \ln(0.375) = -0.9808

t=0.98080.03398=28.9Β minutest = \frac{0.9808}{0.03398} = 28.9 \text{ minutes}

The coffee reaches 120 degrees after about 29 minutes.

Example 3: When will it be within 1 degree of room temperature (73 degrees)?

73=72+128eβˆ’0.03398t73 = 72 + 128e^{-0.03398t}

1=128eβˆ’0.03398t1 = 128e^{-0.03398t}

eβˆ’0.03398t=1128=0.007813e^{-0.03398t} = \frac{1}{128} = 0.007813

βˆ’0.03398t=ln⁑(0.007813)=βˆ’4.852-0.03398t = \ln(0.007813) = -4.852

t=4.8520.03398=142.8Β minutest = \frac{4.852}{0.03398} = 142.8 \text{ minutes}

It takes nearly 2.5 hours to get within 1 degree of room temperature. The last few degrees take a very long time β€” the exponential tail.

Application: Forensic Time of Death

Forensic investigators use Newton’s Law of Cooling to estimate the time of death. Normal body temperature is 98.6 degrees F. After death, the body cools toward the ambient temperature.

Example 4: A body is found at 8:00 PM in a 65-degree room with a temperature of 82 degrees. One hour later, the temperature is 78.5 degrees. Estimate the time of death.

Step 1 β€” Find kk: Let t=0t = 0 be 8:00 PM, so T(0)=82T(0) = 82 and Ts=65T_s = 65.

78.5=65+(82βˆ’65)eβˆ’k78.5 = 65 + (82 - 65)e^{-k}

13.5=17eβˆ’k13.5 = 17e^{-k}

eβˆ’k=13.517=0.7941e^{-k} = \frac{13.5}{17} = 0.7941

k=βˆ’ln⁑(0.7941)=0.2305k = -\ln(0.7941) = 0.2305

Step 2 β€” Find when the body was 98.6 degrees: Now we work backward from the time the body was found. We need the model starting from death, but since we defined t=0t = 0 at 8:00 PM with temperature 82, we need to find when (before 8:00 PM) the temperature was 98.6.

Reset: let T0=98.6T_0 = 98.6 (at death), Ts=65T_s = 65. The model from the time of death is:

T(Ο„)=65+33.6eβˆ’0.2305Ο„T(\tau) = 65 + 33.6e^{-0.2305\tau}

At 8:00 PM (Ο„\tau hours after death), T=82T = 82:

82=65+33.6eβˆ’0.2305Ο„82 = 65 + 33.6e^{-0.2305\tau}

17=33.6eβˆ’0.2305Ο„17 = 33.6e^{-0.2305\tau}

eβˆ’0.2305Ο„=0.5060e^{-0.2305\tau} = 0.5060

βˆ’0.2305Ο„=ln⁑(0.5060)=βˆ’0.6812-0.2305\tau = \ln(0.5060) = -0.6812

Ο„=2.96Β hours\tau = 2.96 \text{ hours}

The person died approximately 3 hours before 8:00 PM β€” around 5:00 PM.

Application: Cooking (Warming Model)

Newton’s Law also models warming. When you put a cold item in a hot environment, the temperature rises toward the ambient temperature.

Example 5: A frozen turkey at 25 degrees F is placed in a 325-degree oven. After 1 hour it is 75 degrees. When will it reach 165 degrees (safe internal temperature)?

Given: T0=25T_0 = 25, Ts=325T_s = 325, T(1)=75T(1) = 75.

Note: T0<TsT_0 < T_s, so (T0βˆ’Ts)=25βˆ’325=βˆ’300(T_0 - T_s) = 25 - 325 = -300. The model is:

T(t)=325βˆ’300eβˆ’ktT(t) = 325 - 300e^{-kt}

Find kk:

75=325βˆ’300eβˆ’k75 = 325 - 300e^{-k}

βˆ’250=βˆ’300eβˆ’k-250 = -300e^{-k}

eβˆ’k=250300=0.8333e^{-k} = \frac{250}{300} = 0.8333

k=βˆ’ln⁑(0.8333)=0.1823k = -\ln(0.8333) = 0.1823

Find tt for T=165T = 165:

165=325βˆ’300eβˆ’0.1823t165 = 325 - 300e^{-0.1823t}

βˆ’160=βˆ’300eβˆ’0.1823t-160 = -300e^{-0.1823t}

eβˆ’0.1823t=160300=0.5333e^{-0.1823t} = \frac{160}{300} = 0.5333

βˆ’0.1823t=ln⁑(0.5333)=βˆ’0.6286-0.1823t = \ln(0.5333) = -0.6286

t=0.62860.1823=3.45Β hourst = \frac{0.6286}{0.1823} = 3.45 \text{ hours}

The turkey reaches 165 degrees after about 3 hours and 27 minutes.

Note: Real cooking is more complex β€” ovens have radiation and convection effects that Newton’s Law simplifies. But the model gives a useful first approximation.

Application: HVAC Engineering

HVAC engineers use Newton’s Law of Cooling to estimate how quickly a building heats or cools after the thermostat is adjusted.

Example 6: An office building is at 68 degrees F when the heating system fails at midnight. The outside temperature is 20 degrees F. The cooling constant for the building is k=0.04k = 0.04 per hour. When will the interior reach 55 degrees?

T(t)=20+(68βˆ’20)eβˆ’0.04t=20+48eβˆ’0.04tT(t) = 20 + (68 - 20)e^{-0.04t} = 20 + 48e^{-0.04t}

55=20+48eβˆ’0.04t55 = 20 + 48e^{-0.04t}

35=48eβˆ’0.04t35 = 48e^{-0.04t}

eβˆ’0.04t=0.7292e^{-0.04t} = 0.7292

βˆ’0.04t=ln⁑(0.7292)=βˆ’0.3158-0.04t = \ln(0.7292) = -0.3158

t=7.9Β hourst = 7.9 \text{ hours}

The building reaches 55 degrees around 7:54 AM β€” before workers typically arrive. The HVAC engineer can use this to plan backup heating or insulation improvements.

Nursing Application: IV Fluid Temperature

In nursing, intravenous fluids sometimes need to reach body temperature before administration. If an IV bag is removed from a 40-degree F refrigerator and placed in a 72-degree room, Newton’s Law models the warming:

T(t)=72+(40βˆ’72)eβˆ’kt=72βˆ’32eβˆ’ktT(t) = 72 + (40 - 72)e^{-kt} = 72 - 32e^{-kt}

With a typical kβ‰ˆ0.1k \approx 0.1 per minute for a standard IV bag, the fluid reaches 65 degrees in:

65=72βˆ’32eβˆ’0.1tβ€…β€ŠβŸΉβ€…β€Š7=32eβˆ’0.1tβ€…β€ŠβŸΉβ€…β€Št=βˆ’ln⁑(7/32)0.1=1.5200.1=15.2Β min65 = 72 - 32e^{-0.1t} \implies 7 = 32e^{-0.1t} \implies t = \frac{-\ln(7/32)}{0.1} = \frac{1.520}{0.1} = 15.2 \text{ min}

Limitations of the Model

Newton’s Law of Cooling assumes:

  • The ambient temperature is constant (if the room heats up from the hot object, the model breaks down)
  • The object has uniform temperature (no hot spots or cold core)
  • Heat transfer is primarily by convection (the model is less accurate for radiation-dominated scenarios)
  • The temperature difference is not extreme (the law is an approximation that works well for moderate temperature ranges)

For precision applications, more sophisticated models (like lumped capacitance or finite element analysis) are used. But for everyday problems β€” coffee cooling, time of death, building heat loss β€” Newton’s Law is remarkably accurate.

Practice Problems

Test your understanding with these problems. Click to reveal each answer.

Problem 1: A pot of soup cools from 212 degrees F to 190 degrees in 10 minutes in a 70-degree kitchen. Find kk and determine when the soup reaches 140 degrees.

190=70+142eβˆ’10k190 = 70 + 142e^{-10k}

120=142eβˆ’10k120 = 142e^{-10k}

eβˆ’10k=0.8451e^{-10k} = 0.8451

k=βˆ’ln⁑(0.8451)10=0.168310=0.01683k = \frac{-\ln(0.8451)}{10} = \frac{0.1683}{10} = 0.01683

When is T=140T = 140?

140=70+142eβˆ’0.01683t140 = 70 + 142e^{-0.01683t}

70=142eβˆ’0.01683t70 = 142e^{-0.01683t}

eβˆ’0.01683t=0.4930e^{-0.01683t} = 0.4930

t=βˆ’ln⁑(0.4930)0.01683=0.70720.01683=42.0Β minutest = \frac{-\ln(0.4930)}{0.01683} = \frac{0.7072}{0.01683} = 42.0 \text{ minutes}

Answer: k=0.01683k = 0.01683; the soup reaches 140 degrees in about 42 minutes.

Problem 2: A cold beverage at 38 degrees F is placed in an 80-degree room. After 15 minutes it is 50 degrees. When does it reach 70 degrees?

50=80+(38βˆ’80)eβˆ’15k=80βˆ’42eβˆ’15k50 = 80 + (38 - 80)e^{-15k} = 80 - 42e^{-15k}

βˆ’30=βˆ’42eβˆ’15k-30 = -42e^{-15k}

eβˆ’15k=0.7143e^{-15k} = 0.7143

k=βˆ’ln⁑(0.7143)15=0.336515=0.02243k = \frac{-\ln(0.7143)}{15} = \frac{0.3365}{15} = 0.02243

For T=70T = 70:

70=80βˆ’42eβˆ’0.02243t70 = 80 - 42e^{-0.02243t}

10=42eβˆ’0.02243t10 = 42e^{-0.02243t}

t=βˆ’ln⁑(10/42)0.02243=1.43510.02243=64.0Β minutest = \frac{-\ln(10/42)}{0.02243} = \frac{1.4351}{0.02243} = 64.0 \text{ minutes}

Answer: The beverage reaches 70 degrees in about 64 minutes (just over 1 hour).

Problem 3: A body is found at 10:00 AM in a 60-degree room at 85 degrees F. At 11:00 AM, the body is 80 degrees. Estimate time of death.

Find kk from the 10-11 AM data: T(0)=85T(0) = 85, Ts=60T_s = 60, T(1)=80T(1) = 80:

80=60+25eβˆ’kβ€…β€ŠβŸΉβ€…β€Š20=25eβˆ’kβ€…β€ŠβŸΉβ€…β€Šk=βˆ’ln⁑(0.8)=0.223180 = 60 + 25e^{-k} \implies 20 = 25e^{-k} \implies k = -\ln(0.8) = 0.2231

Now find hours before 10 AM when body was 98.6:

T(Ο„)=60+38.6eβˆ’0.2231Ο„T(\tau) = 60 + 38.6e^{-0.2231\tau}

85=60+38.6eβˆ’0.2231Ο„85 = 60 + 38.6e^{-0.2231\tau}

25=38.6eβˆ’0.2231Ο„25 = 38.6e^{-0.2231\tau}

eβˆ’0.2231Ο„=0.6477e^{-0.2231\tau} = 0.6477

Ο„=βˆ’ln⁑(0.6477)0.2231=0.43430.2231=1.95Β hours\tau = \frac{-\ln(0.6477)}{0.2231} = \frac{0.4343}{0.2231} = 1.95 \text{ hours}

Answer: Death occurred about 2 hours before 10 AM, around 8:00 AM.

Problem 4: An HVAC system can maintain k=0.02k = 0.02 per hour for a well-insulated building. If the inside is 72 degrees and the outside drops to 10 degrees, how long until the interior reaches 60 degrees (if the heating fails)?

60=10+62eβˆ’0.02t60 = 10 + 62e^{-0.02t}

50=62eβˆ’0.02t50 = 62e^{-0.02t}

eβˆ’0.02t=0.8065e^{-0.02t} = 0.8065

t=βˆ’ln⁑(0.8065)0.02=0.21510.02=10.75Β hourst = \frac{-\ln(0.8065)}{0.02} = \frac{0.2151}{0.02} = 10.75 \text{ hours}

Answer: About 10 hours and 45 minutes until the building drops to 60 degrees. The good insulation (small kk) buys time.

Problem 5: Two cups of coffee start at 200 degrees F in a 70-degree room. Cup A (ceramic) has k=0.03k = 0.03 and Cup B (insulated mug) has k=0.01k = 0.01. After 30 minutes, what are their temperatures?

Cup A: T(30)=70+130eβˆ’0.03Γ—30=70+130eβˆ’0.9=70+130Γ—0.4066=70+52.9=122.9T(30) = 70 + 130e^{-0.03 \times 30} = 70 + 130e^{-0.9} = 70 + 130 \times 0.4066 = 70 + 52.9 = 122.9 degrees

Cup B: T(30)=70+130eβˆ’0.01Γ—30=70+130eβˆ’0.3=70+130Γ—0.7408=70+96.3=166.3T(30) = 70 + 130e^{-0.01 \times 30} = 70 + 130e^{-0.3} = 70 + 130 \times 0.7408 = 70 + 96.3 = 166.3 degrees

Answer: After 30 minutes, the ceramic cup is about 123 degrees and the insulated mug is about 166 degrees β€” a 43-degree difference. Insulation matters.

Key Takeaways

  • Newton’s Law of Cooling: T(t)=Ts+(T0βˆ’Ts)eβˆ’ktT(t) = T_s + (T_0 - T_s)e^{-kt} β€” temperature approaches ambient exponentially
  • The formula works for both cooling (T0>TsT_0 > T_s) and warming (T0<TsT_0 < T_s)
  • The constant kk is found from a known temperature at a known time β€” it depends on material properties and environment
  • A larger kk means faster temperature change (poor insulation); smaller kk means slower change (good insulation)
  • Applications include forensics (time of death), cooking, HVAC (building heat loss), and nursing (fluid warming)
  • The model assumes constant ambient temperature and uniform object temperature

Return to College Algebra for more topics in this section.

Last updated: March 29, 2026