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Heat and Entropy

Heat transfer and throttling

Why coffee cools and laptops slow down

Start a heavy game or a long compile and your laptop is quick for about half a minute, then the fan roars and everything gets slower - even though the code has not changed and the battery is full. Nothing broke. The chip walked into a physical wall it cannot cross: it is making heat faster than it can get rid of it. To understand why, we follow the heat on its journey from the silicon to the room.

Predict first: what fixes overheating?

A friend says their laptop throttles under load and they are going to fix it with a much bigger, faster fan. Before reading on, predict: will a bigger fan alone reliably solve it? Hold your guess. The answer is often no, and the reason is that heat crosses several barriers in a row, and the fan only speeds up the last one - the slowest barrier in the chain sets the ceiling.

Three ways heat moves

Before any of this, heat needs a way to travel. There are exactly three, and you have felt all of them.

Conduction: touch

Energy passes molecule to molecule through direct contact, fast jigglers bumping slow neighbors. A metal spoon left in hot soup grows warm at the handle you never dipped. This is how heat leaves a chip through the metal pressed against it.

Convection: flow

A moving fluid carries heat away bodily. Boiling water churns; a fan drags warm air off a surface and replaces it with cool air. This is the fan's whole job.

Radiation: glow

Every warm object beams energy as invisible infrared light, needing no contact and no air at all. It is how the Sun's heat crosses empty space to you and how a campfire warms your face across the gap. For a warm chip it is a minor channel, but it never fully switches off.[1]

One thing all three share: heat only ever flows from hotter to colder, never the reverse on its own. "Cold" does not flow into a warm room through an open freezer - warm air flows out. There is no cold; there is only more heat and less heat, and it always drains downhill in temperature. That one-way rule is the seed of the next lesson.

Play: the heat's journey off the chip

Here is the path heat takes from a running CPU to the room, drawn as a stack. The chip pours out a fixed number of watts; that power has to climb through the paste, the heatsink, and the fan-stirred air to escape. Turn the chip power up, or make any layer worse, and watch the junction temperature at the bottom climb toward the throttle line.

The chip's heat crosses three resistances in series to reach the air: paste, heatsink, and the fan-stirred film. Junction temperature is just 25 + P × R. Push it past the throttle line and the chip cuts its own power to survive - performance falls.
room air25 Cheatsink fins50 Cheatsink base56 Cthermal paste62 CCPU die68 CR paste0.27 K/WR heatsink0.14 K/WR convection0.55 K/Wthrottle 95 C68 C
junction temp
68 C
R total
0.96 K/W
clock
4.0 GHz
status
nominal

Now the predict probe resolves. Crank the fan to full and the junction temperature drops only a little if the paste is the weak link - because the fan only improves the last hop. The heat still has to crawl through whatever the worst layer is first. The bottleneck is set by the largest barrier in the chain, not by the fastest one.

Heat flow is Ohm's law in disguise

Newton noticed the simplest version of this centuries ago: an object cools at a rate proportional to how much hotter it is than its surroundings. Turn that around and it says the temperature gap needed to push a given flow of heat is proportional to the heat flow. Define the constant of proportionality as a and you get a clean law:

Stated (Newton's law of cooling, rearranged): the temperature drop across a layer equals the heat flow times the layer's thermal resistance.

If that shape looks familiar, it should. It is exactly from electric circuits, with temperature difference playing the role of voltage, heat flow playing the role of current, and thermal resistance playing the role of electrical resistance. The analogy is not a loose metaphor; the equations are identical, which is why engineers draw cooling systems as resistor networks.[2]

And here is the part the widget makes vivid: the layers sit in series - paste, then heatsink, then air - and resistances in series add, just like resistors in a wire. The total temperature the chip runs above the room is the sum of the drops across every layer:

Derived by stacking the per-layer drops: the junction rides above ambient by the total resistance times the power.

Because the resistances add, the worst layer dominates the sum. A brilliant fan (tiny ) cannot rescue a chip choked by dried cracked paste (huge ). The chain is only as good as its worst link.

Why the laptop slows down

Everything connects now. In power and efficiency we saw that a chip turns nearly all the electrical power it draws into heat: a 45 watt CPU is a 45 watt heater. That is the heat flow in the equation above, and the faster the chip runs, the more power it burns and the more heat it must shed.

The chip has a temperature it must not exceed or it will be damaged. When the steady-state junction temperature would climb past that limit, the chip protects itself by : it lowers its own clock speed and voltage, which cuts , which pins the temperature at the limit. Your frame rate drops, your compile slows, and the chip survives. The thirty-second head start is the time it takes the heatsink to soak up heat and reach that ceiling; after that, the cooling chain, not the silicon, sets your speed.[3]

The everyday face of the power wall

Thermal throttling is the daily, personal version of a much bigger story. The reason CPUs stopped simply getting faster around 2005 - the power wall - is this same heat-out-of-a-resistance-chain problem at the scale of the whole industry. Your laptop hitting its limit and the end of ever-rising clock speeds are the same physics.
T_air   = 25.0     # ambient, Celsius
limit   = 95.0     # junction temperature the chip must not exceed

# Thermal resistances in series (kelvin per watt). They ADD, like resistors.
R_paste, R_heatsink, R_air = 0.10, 0.14, 0.35
R_total = R_paste + R_heatsink + R_air

def junction_temp(power_watts):
    return T_air + power_watts * R_total     # deltaT = P * R

requested = 65.0
if junction_temp(requested) > limit:
    # Throttle: cap power so the junction sits exactly at the limit.
    allowed = (limit - T_air) / R_total
    performance = allowed / requested        # fraction of full speed
    print(f"throttling to {performance:.0%} of full speed")
else:
    print("running at full speed")
The steady-state junction temperature and the throttle decision, in a few lines.

Lock it in

  • Heat moves three ways: conduction (touch), convection (flowing fluid), and radiation (infrared glow). It always flows hot to cold, never the reverse on its own.
  • Heat flow obeys , the exact shape of Ohm's law . Temperature gap is like voltage, heat flow like current, thermal resistance like electrical resistance.
  • The cooling layers sit in series, so their resistances add. The worst layer dominates - a great fan cannot save bad paste.
  • A chip is a heater: its power becomes heat crossing that chain. When the junction would pass its safe limit, it throttles - drops clock speed to cut heat - and your performance falls.
  • The thirty-seconds-then-slow feeling is the heatsink warming up to its ceiling; after that the cooling chain sets the speed. It is the everyday face of the power wall.

Check yourself

Your laptop runs a game fast for about thirty seconds, then noticeably slows and the fan gets loud. What physical limit did it hit?

This is the lesson's anchor - name the mechanism, not just the symptom. Try to state it, then check.

Heat always flows...

A CPU throttles - lowers its clock speed - in order to...

Match each mode of heat transfer to an everyday example.

drop here

a chip's heat crossing the metal heatsink pressed to it

drop here

a fan dragging warm air away and pulling cool air in

drop here

a campfire warming your face across the gap

Primary source

Feynman Lectures on Physics, Vol I Ch 44: The Laws of Thermodynamics

Feynman treats heat flow and the direction it must run, setting up why the one-way rule matters. Pair it with any datasheet's thermal-resistance table to see engineers use exactly as this lesson does.

Sources

  1. 1.Feynman Lectures Vol I Ch 44, The Laws of Thermodynamics
  2. 2.OpenStax University Physics Vol 2, Ch 1: Temperature and Heat
  3. 3.Dynamic frequency scaling (thermal throttling), Wikipedia