Energy Balance

Based on the 1st law, more specific equations are derived on a case by case basis.

Transient State

When a thermodynamic system’s state and energy transfer changes with time.

Steady State

When a thermodynamic system’s state constants with time. Net energy change in the system is zero.

For Closed Systems

Net energy transfer to a closed system is equal to the net increase in the system’s total energy.

ΔQ−ΔW=ΔEsys=ΔU+ΔKE+ΔPEΔU=m(h2−h1)ΔKE=12m(C22−C12)ΔPE=mg(z2−z1)\begin{equation} \nonumber \begin{split} \Delta Q - \Delta W & = \Delta E_{\text{sys}} = \Delta U + \Delta KE + \Delta PE \\ \Delta U & = m(h_2 - h_1) \\ \Delta KE & = \frac{1}{2}m \left(C_2^2 - C_1^2\right) \\ \Delta PE & = mg(z_2 - z_1) \end{split} \end{equation}
Here:
ΔQ\Delta Q
net heat transfer to the system
ΔW\Delta W
net work transfer from the system
ΔEsys\Delta E_{\text{sys}}
change in total energy
ΔU\Delta U
change in internal energy
ΔKE\Delta KE
change in kinetic energy
ΔPE\Delta PE
change in potential energy
h1,h2h_1, h_2
specific enthalpy
mm
mass of the system
C1,C2C_1, C_2
velocity of the system
gg
gravitational acceleration
z1,z2z_1, z_2
elevation of the system

For Open Systems

Total specific energy of a flow system:

θ=h+12C2+gz\theta = h + \frac{1}{2}C^2 + gz
Here:
θ\theta
total specific energy
h=u+Pνh = u + P\nu
enthalpy
uu
specific internal energy
PνP\nu
specific flow work
CC
velocity of the flow
gg
gravatitaional acceleration
zz
elevation of the flow system

The energy balance is:

Q−W+minθin−moutθout=ΔEsysQ - W + m_{\text{in}}\theta_{\text{in}} - m_{\text{out}}\theta_{\text{out}} = \Delta E_{\text{sys}}
Here:
QQ
heat transfer
WW
work transfer
minm_{\text{in}}
mass flow rate of the inlet
θin\theta_{\text{in}}
total specific energy of the inlet
moutm_{\text{out}}
mass flow rate of the outlet
θout\theta_{\text{out}}
total specific energy of the outlet
ΔEsys\Delta E_{\text{sys}}
change in total energy of the system

Steady Flow Energy Equation (SFEE)

Used when an open system is in steady state.

q−w=he−hi+12(Ce2−Ci2)+g(ze−zi)q - w = h_e - h_i + \frac{1}{2}\Big(C_e^2 - C_i^2\Big) + g(z_e - z_i)
Here:
qq
specific heat transfer
ww
specific work transfer
he,hih_e, h_i
specific enthalpy at the outlet and inlet
Ce,CiC_e, C_i
flow velocity at the outlet and inlet
gg
gravitational acceleration
ze,ziz_e,z_i
elevation at the outlet and inlet
Written by November 3, 2026 2 min read
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