Notes for Examination
Temperature
Relation between Celsius and fahrenhite scale is
TF=9/5 TC + 32°
TF - Fahrenhite Temperature
TC - Celsius Temperature
Relation between Celsius and kelvin scale is
TC = TK - 273.15 K
TK - Temperature in Kelvin
TC - Temperature in celsius
- If R0 & R100 are resistance of metak wire at ice and steam point resp then temp t can be defined corresponding to resistance RT as follows
- The pressure,volume and temperature in kelvin of such gases obey the equation
PV=nRT ----(1)
Thermal expansion
ΔL=αLΔT
Specific Heat Capacity
Gas Laws
Boyles Law: PV=constant
Charles Law : V/T=constant
Dalton Law of Partial Pressure: P=P1 + P2 +P3
Root mean Square VelocityVrms=√3RT/M
Mean Square Velocity
Vm=√8RT/πM
Average Velocity
V=√2RT/M
Also
Vrms > Vm > V
Average kinetic Energy of Gas=3/2nRT
First law of Thermodynamics
ΔU=Q-W
Gas Processes
Isothermal Process : PV=constant ,ΔU=0,Q=W,Molar Specific Heat=infinity
Adaibatic Process : PVy=constant,Q=0,ΔU=-W,Molar Specific Heat=zero
Polytropic Process : PVn=constant,Molar Specific Heat=R/y-1 + R/1-n
Volume Constant : P/T=constant W=0,ΔU=Q,Molar Specific Heat=Cv
Pressure Constant : V/T=constant ΔU=Q-W ,Molar Specific Heat=CP
Internal energy depends on Temperature.
So for same temperature change ΔT
nCvΔT=Q1-W1=Q2-W2=Q3-W3
Molar Specfic Heat Capacity of any process is given by
C=Cv + Pdv/ndT where n is no of moles of the gas
Workdone by Gas= ∫PdV
Heat Conduction
Q=-KAdT/dx
Wein displacement lawλT4=Constant
Stefan's Law
Q=eσT4
Newton law of Cooling
dT/dx=b(T-Ts)
Temperature
Relation between Celsius and fahrenhite scale is
TF=9/5 TC + 32°
TF - Fahrenhite Temperature
TC - Celsius Temperature
Relation between Celsius and kelvin scale is
TC = TK - 273.15 K
TK - Temperature in Kelvin
TC - Temperature in celsius
- If R0 & R100 are resistance of metak wire at ice and steam point resp then temp t can be defined corresponding to resistance RT as follows
T = | (RT-R0)*100 |
R100-R0 |
- The pressure,volume and temperature in kelvin of such gases obey the equation
PV=nRT ----(1)
Thermal expansion
ΔL=αLΔT
Specific Heat Capacity
c = | `Q |
nΔT |
Gas Laws
Boyles Law: PV=constant
Charles Law : V/T=constant
Dalton Law of Partial Pressure: P=P1 + P2 +P3
Root mean Square VelocityVrms=√3RT/M
Mean Square Velocity
Vm=√8RT/πM
Average Velocity
V=√2RT/M
Also
Vrms > Vm > V
Average kinetic Energy of Gas=3/2nRT
First law of Thermodynamics
ΔU=Q-W
Gas Processes
Isothermal Process : PV=constant ,ΔU=0,Q=W,Molar Specific Heat=infinity
Adaibatic Process : PVy=constant,Q=0,ΔU=-W,Molar Specific Heat=zero
Polytropic Process : PVn=constant,Molar Specific Heat=R/y-1 + R/1-n
Volume Constant : P/T=constant W=0,ΔU=Q,Molar Specific Heat=Cv
Pressure Constant : V/T=constant ΔU=Q-W ,Molar Specific Heat=CP
Internal energy depends on Temperature.
So for same temperature change ΔT
nCvΔT=Q1-W1=Q2-W2=Q3-W3
Molar Specfic Heat Capacity of any process is given by
C=Cv + Pdv/ndT where n is no of moles of the gas
Workdone by Gas= ∫PdV
Heat Conduction
Q=-KAdT/dx
Wein displacement lawλT4=Constant
Stefan's Law
Q=eσT4
Newton law of Cooling
dT/dx=b(T-Ts)
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