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Instrument MI-03-417 · Physics

Sensible Heat Calculator

Not every joule you add makes something hotter — sensible heat is the part that does. Enter mass, specific heat and a temperature change to see the cost.

Instrument MI-03-417
Sheet 1 OF 1
Rev A
Verified
Type 03 — Thermal SER. 2026-03417

Sensible heat

201,200.000000 J

Q = m·c_p·ΔT

The working Every figure verified twice
  1. Q = 10·1006·20 = 201,200.000000
Worksheet log
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How this instrument works

Sensible heat is the energy that changes an object's temperature without changing what phase it is in — solid, liquid or gas stays put while the thermometer moves. The name is literal: this is the portion of heat a thermometer can actually sense, in contrast to latent heat, which rearranges molecular bonds during melting, boiling or freezing while the reading holds still. The formula Q = m·cp·ΔT says the energy scales three ways at once: double the mass and you double the bill, double the temperature swing and you double it again, and cp sets how expensive that swing is for whatever material sits in front of you.

The constant is written cp rather than plain c because this instrument is built around processes that happen at roughly constant pressure — air moving through a duct, a room or the open atmosphere is always free to expand against whatever surrounds it, unlike a gas trapped in a sealed tank. Dry air's cp, about 1006 J/(kg·K), sits in the Specific heat field by default because warming and cooling air is the single most common use of this equation in building-services work: an air-handling engineer sizing a heating coil runs exactly this multiplication, only with mass expressed as a flow of air rather than one fixed batch.

The formula assumes cp stays fixed across the interval and that no moisture condenses or evaporates along the way. Cool a humid air stream far enough and it starts shedding water as it goes; part of the energy budget then quietly becomes latent heat, which this equation cannot see. Meteorologists lean on the same split at the scale of a whole landscape: incoming solar energy at the ground divides into a sensible flux that warms the air directly and a latent flux that evaporates water instead, and that ratio — the Bowen ratio — is why a parched desert afternoon can feel scorching while a wetland under an equally strong sun stays comparatively mild.

Q=mcpΔTQ = m \, c_p \, \Delta T
Q — sensible heat, joules (J) · m — mass, kilograms (kg) · cp — specific heat at constant pressure, joules per kilogram-kelvin (J/(kg·K)) · ΔT — temperature change, °C, a step equal in size to one kelvin, so no conversion between the two is needed.
  • Enter the quantity of material into Mass — kilograms, grams or pounds all convert automatically.
  • Set Specific heat, J/(kg·K) to your material's constant; 1006 is already filled in for dry air, or swap in water's 4186, or any other tabulated figure.
  • Enter Temperature change, °C as the rise you expect, positive, or the drop, negative — a difference, never a single reading.
  • Read Sensible heat, switching between joules and kilojoules to match a lab notebook or a load calculation.
  • A negative Temperature change returns a negative Sensible heat — energy the material is giving up, the shape a cooling-coil load takes.

Worked example — warming 10 kg of dry air by 20 °C

An air-handling engineer is sizing a duct heater that must lift 10 kg of dry air by 20 °C before it reaches a room. Mass = 10, Specific heat, J/(kg·K) = 1006, the default value for dry air, and Temperature change, °C = 20. Multiplying straight through: Q = 10 × 1006 × 20 = 201,200 J, which the Sensible heat field also reads back as 201.2 kJ.

Spread across one minute of steady operation, 201,200 J works out to about 3,353 W, roughly what a kettle and a toaster draw running together — a handy way to sanity-check a coil's rated wattage against a textbook multiplication. None of that energy touches the air's moisture content; if the same stream also needed dehumidifying, that separate latent load would sit on its own line of the total heating or cooling capacity, never folded into this figure.

Questions

What is the difference between sensible heat and latent heat?

Sensible heat changes temperature; latent heat changes phase while temperature holds still. A pot of water climbing from 20 °C to 100 °C is absorbing sensible heat the whole way, following Q = m·cp·ΔT. Once it starts boiling, every further joule goes into freeing molecules from the liquid instead, and the thermometer stops moving entirely — that energy is latent, and belongs to a different relation, Q = m·L, not this one.

Why does this instrument use cp instead of the cv you might remember from chemistry?

Because almost everything it is built for — air in a duct, a room, or the open atmosphere — is free to expand against roughly constant pressure as it warms, and cp is the specific heat that accounts for that expansion work. cv, near 0.718 kJ/(kg·K) for dry air against cp's 1.006 kJ/(kg·K), applies only to gas sealed inside a fixed volume, such as a rigid pressure vessel, a situation this instrument was not built to model.

How is a sensible heat calculation different from a plain specific-heat one?

The equation is the same multiplication, m·c·ΔT, wearing a different label. Engineers reach for the name 'sensible heat' specifically when the material is air and the context is a building, duct or atmosphere — a label that exists mainly to separate the result from the latent heat spent on humidity, a distinction a general specific-heat problem usually does not need to make.

What is the sensible heat ratio, and where does this figure fit into it?

The sensible heat ratio (SHR) is sensible heat divided by total heat, sensible plus latent, for an air-conditioning load — typically 0.65 to 0.80 for a home in a humid climate. This calculator produces the sensible half of that fraction; the latent half comes from a separate moisture-removal calculation, and equipment gets picked so its own rated SHR matches the room's, or it over-cools the air while barely touching the humidity.

Does 'sensible heat' mean the same thing to a meteorologist?

Yes, the same physics, applied to a whole landscape rather than a duct. Solar energy reaching the ground splits into a sensible heat flux that warms the air directly and a latent heat flux that evaporates water instead; their ratio, the Bowen ratio, is why a dry desert afternoon can feel scorching, since nearly all the energy raises air temperature, while a wetland under the same sun stays milder because most of it goes into evaporation.

References