Measurement of Heat Energy
Heat is a form of energy called thermal energy that flows due to temperature difference. It is measured in joules.
The quantity of heat Q received by a body is proportional to its mass (m), and temperature change (02 – 01) and on the nature of the material the body is made of.
Thus Q∝(θ2−θ1)Q=MC(θ2−θ1)
C is a constant of proportionality called the specific heat capacity of the body, which depends on the nature of the body.
The quantity of heat energy possessed by a body depends on these three quantities:
(i) the change in temperature (θ2 – θ1)
(ii) the specific heat capacity of the body (C)
(iii) mass of the body (m)
Heat Capacity
This is the quantity of heat required to raise the temperature of the entire body by one degree rise in temperature(1k). It is measured in Joules/K.
H = MC
Specific Heat Capacity
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Specific heat capacity of a substance is the heat required to raise the temperature of a unit mass(1kg) of the substance through a degree rise in temperature(10C or 1K)
Q=MC(θ2−θ1)
Q is quantity of heat, C is specific heat capacity, (θ2−θ1) change in temperature and m is the mass of the substance.
C=QM(θ2−θ1)
The unit is JKg-1K-1
Example 1:
What is meant by the statement: The specific heat capacity of copper is 400Jkg-1k-1?
Solution:
It means the quantity of heat required to raise the temperature of a unit mass of copper through one degree rise in temperature is 400J
Example 2:
How much heat is given out when a piece of iron of mass 50g and specific heat capacity 460Jkg-1K-1 cools from to 250C.
Solution:
M=50g=0.05kg,=460Jkg−1k−1,θ2−θ1=85−25=60oCQ=MC(θ2−θ1)Q=0.05×460×60=1380J
Determination of the Specific Heat Capacity of a Solid by Method of Mixtures
The solid lead block is weighed on a balance to be M1. A lagged calorimeter is dried and weighed to be M2. It is then reweighed to be M3 when half filled with water. The initial temperature of the water is taken to be 01.
The lead block is suspended in boiling water with a temperature 02 after which it is transferred to the calorimeter and the mixture stirred to maintain a uniform temperature 03.
The specific heat capacity of the lead can be calculated using the fact that heat loss by the lead = heat gained by calorimeter and water. Given the specific heat capacity of calorimeter and water to be Cc and Cw respectively.
M1Cc(θ2−θ3)=M2Cc(θ3−θ1)+(M3−M2)Cw((θ3−θ1))C1=(M2Cc)(θ3−θ1)+(M3−M2)Cw(θ3−θ1)M1(θ2−θ3) |
Precautions:
Calculations Using Method of Mixtures
Example 3:
An iron rod of mass 2kg and at a temperature of 2800C is dropped into some quantity of water initially at a temperature of 300C . If the temperature of the mixture is 700C , calculate the mass of the water. [Neglect heat losses to the surroundings.] [Specific heat capacity of iron = 460Jkg-1K-1, Specific heat capacity of water = 4200Jkg-1K–]
Solution:
Mass of iron rod = M1 = 2kg
Temperature of hot iron rod = θ2 = 2800C
Initial temperature of water = θ1 = 30oC
Final temperature of mixture = θ3 = 700
Specific heat capacity of iron = CI = 460Jkg-1K-1
Mass of water = M2 = ?
Heat lost by hot iron = heat gained by water
M1CI(θ2−θ3)=M2CW(θ3−θ1)M2=M1CI(θ2−θ3)CW(θ3−θ1)M2=2×460×(280−70)4200(70−30)M2=2×460×2104200×40M2=193200168000=1.15kg
Example 4:
A piece of copper of mass 120g is heated in an enclosure to a temperature of 1250C. it is then taken out of the enclosure and held in air for half a minute and dropped carefully into a copper calorimeter of mass 105g containing 200g of water at 200C. The temperature of the water rises to 250C. Calculate the rate at which heat is being lost from the piece of copper when it is held in air. (specific heat capacity of water is 4200Jkg – 1 0C – 1 , specific heat capacity of copper is 400J kg – 10C – 1 WAEC)
Solution:
θ1 = 1250C, θ2 = 250C, mass of copper (Mc) = 120g = (120/1000)kg = 0.12kg
Heat lost by copper =McCc(θ2−θ1)=0.12×400×(125−25)=480J
Mass of calorimeter (mc) =105g=(1051000)kg=0.105kg
Specific heat capacity of calorimeter (cc) =400Jkg−10C−1
Mass of water =(2001000)kg=0.2kg
Change in temperature Δθ=(25−20)oC
Heat gained by calorimeter and water
=McCcΔθ+MwCwΔθ=0.105×400×(25−20)+0.2×4200×(25−20)=4410J |
Heat lost to air =4800−4410=390J
Therefore, rate of lost of heat to air
=39030=13Js−1
To calculate the specific heat capacity Cb of a solid brass block, we make two holes in a weighed brass block into which a thermometer and a heating element connected to a source of power supply are inserted. Oil is poured in the holes to ensure thermal conductivity. Assuming no heat is lost to the surrounding, the total amount of electrical heat energy supplied by the coil, Ivt = heat gained by the brass, MCb0
Ivt=MCbθ ——(1)
From v = IR (Ohms law)
I2Rt=MCbθ ——(2)
v2tR=MCbθ ——(3)
Example 5:
A liquid of specific heat capacity 3Jg – 1 k – 1 rises from 150C to 650C in one minute when an electric heater is used. If the heater generates 63KJ per minute, calculate the mass of the liquid.
Solution:
Specific heat capacity of liquid
C1=3Jg−1k−1=3000Jkg−1k−1Δθ=65−15=50oC
Heat supplied by heater = heat gained by water
Ivt = Ml x Cl Δθ where Ml = mass of liquid
63000=M1×3000×50M1=630003000×50=0.42kg
Example 6: A certain metal of mass 1.5kg at initial temperature of 270C, absorb heat from electric heater of 75W rating for 4 minutes. If the final temperature was 470C, calculate the specific heat capacity of the metal and its heat capacity.
Solution:
Time ‘t’ = 4 minutes = 4 × 60 = 240s. power IV = 75W, mass of metal ‘m’ = 1.5kg.
Heat supplied by electric heater = heat gained by the metal
IVt=mcΔθ75×240=1.5×c×(47–27)75×240=1.5×c×20c=75×2401.5×20=600Jkg−1K−1
Heat capacity =mc=1.5×600=900JK−1
GENERAL EVALUATION ( POST YOUR ANSWER IN THE COMMENT BOX AT THE BOTTOM FOR RATING AND DISCUSSION)
Determination of Specific Heat Capacity of Liquid by Electrical Method
Apparatus:
Thermometer, liquid, calorimeter, heater, stop clock, chemical/beam balance
Method:
A calorimeter of known heat capacity (McCc) is used and a known mass of liquid( M1) is placed in the calorimeter, the temperature of the liquid is recorded (θ1)). The known quantity of heat (VIt) is recorded by taking readings from the voltmeter, ammeter and stop watch. The final temperature is recorded (θ2).
Calculations:
Electrical energy supplied by the heater = Heat energy absorbed by the calorimeter and water.
VIt=M1CL(θ2−θ1)+McCc(θ2−θ1)CL=VIt−McCc(θ2−θ1)C1(θ2−θ1) |
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