thermal physics Flashcards
definition of specific heat capacity
energy required to raise the temperature of 1kg of a substance by 1 Kelvin
units of specific heat capacity
J kg-1 K-1
experiment to calculate specific heat capacity
Continuous flow calorimeter:
1)Set up the experiment with a heating element heating the water and let the water flow at a steady rate until the water out is at a constant temperature.
2)Record the flow rate of the water and duration of the experiment to find the mass of the water as well as the temperature difference (∆θ) between the water in and water out.
3)Record the current and p.d to find the energy transferred to the water (E=IVt+H where H is the heat lost to the surroundings.
4)Repeat the experiment only changing the p.d of the power supply and flow rate (mass) so ∆θ remains constant. You should now have an equation for each experiment.
5)Rearrange equations to get
c=Q₂-Q₁ / (m₂-m₁)∆θ as the H’s cancel.
6) Use Q=IVt to find Q₁ and Q₂ to find the specific heat capacity.
specific latent heat
the energy required to change the state of 1 kg of a substance without raising its temperature
what happens during a change of state
- there is no change in temperature
- kinetic energies of particles are constant
- the potential energies of particles are changing
definition of specific latent heat of vapourisation
the energy required to change the state of 1 kg of a substance from liquid to gas without changing its temperature
definition of specific latent heat of fusion
energy required to change the state of 1 kg of substance from solid to liquid without changing its temperature
Units of specific latent heat
Jkg-1
definition of absolute zero
temperature at which there is zero kinetic energy per particle
absolute zero in degrees celsius
-273 degrees
converting between Kelvin and Celsius temperature scales
Kelvin to Celsius: subtract 273
Celsius to Kelvin: add 273
pressure volume graph
- pressure is proportional to 1/volume so an increased temperature or mass of gas causes the curve to move right and up.
- use pV=nRT to determine changes to graphs
pressure-temperature graph
- temperature is in Kelvin
- pressure is proportional to T
- decreasing the volume or increasing the mass of gas caused a steeper gradient
- use pV=nRT to determine changes to graphs
volume-temperature graph
- temperature is in Kelvin
- V is proportional to T
- decreasing the pressure or increasing the mass of gas caused a steeper gradient
- use pV=nRT to determine changes to graphs
why might energy put into a material not equal the specific heat capacity calculated
energy lost to surroundings means specific heat capacity may not be constant over the temperature range used
define terms N, m and crms in pV = ⅓Nm(crms2).
N - number of particles(molecules)
m - mass of individual particles (molecules)
crms - square root of mean square speed
average kinetic energy per particle of a gas at temperature
=3/2kT = 1/2m(Crms²)
k - boltzman constant - 1.38x10^-23
Total kinetic energy of gas at temperature T
= N x 1.5kT = N x 0.5mCrms². Where N is the number of particles/molecules in gas
k - boltzman constant - 1.38x10^-23