Units is usually 1J(Joule)=1NNewton⋅1mmetre; or 1J=1kg⋅1m2/1s2
Principal of conservation of energy
Energy cannot be created or destroyed
only transferred from one store to another
The total amount of energy in a system is constant
Work Done
the amount of energy transferred when a force moves an object over a distance
Work done=FdwhereFdforce in the direction of displacement in newtonsdisplacement in metres
Power
The rate at which work is done or energy is transferred over time
P=tWwherePWtpower in W (watt)work done in Joulestime taken in secondsP=tΔEwhereΔEtchange in energy (or energy transferred) in Joulestime taken in seconds
Instatenous power
\begin{align*}
P &= \frac{W}{t} \\
&= \frac{Fd}{t} \\
&= F(\frac{d}{t}) \\
&= Fv \\
&\hspace{-5em} \rlap{\text{\textbf{where}}}\phantom{P} & \\
&\hspace{-5em} \rlap{\quad \begin{array}{rl}
F & \text{force in Newtons} \\
v & \text{velocity or speed in metres per second}
\end{array}}\phantom{P} &
\end{align*}
Stores of energy
kinetic store
\begin{align*}
E_k &= \frac{1}{2}mv^2 \\
&= \frac{1}{2}pQv^2 \\
& \hspace{-5em} \rlap{\text{\textbf{where}}}\phantom{E_k} & \\
& \hspace{-5em} \rlap{\quad \begin{array}{rl}
m & \text{mass in Kilograms} \\
v & \text{velocity in metres per second} \\
p & \text{density of water in $Kg/m^3$} \\
Q & \text{volumetric flow rate in $m^3/s$} \\
\end{array}}\phantom{E_k} &
\end{align*}v=AQwherevQAfluid velocity in ms−1volumetric flow rate in mcross-sectional area in
gravitational potential store
Ep=mghwheremghmass in Kilogramsacceleration due to gravityheigh in metres
elastic potential store
\begin{align*}
E_e &= \frac{1}{2}kx^2 \\
& \hspace{-5em} \rlap{\text{\textbf{where}}}\phantom{E_e} & \\
& \hspace{-5em} \rlap{\quad \begin{array}{rl}
k & \text{spring constant in newtons per metre ($N/m$)} \\
x & \text{extension in metres}
\end{array}}\phantom{E_e} &
\end{align*}
chemical potential store
Internal store
nuclear store
means of energy transfer
Mechanically -> force
Propagation of waves (eg sound waves)
Heating (2 different temperatures)
Electrical
P=J/swherePRtotal energy or work done in joules (J)
Work Energy Theorem
the net work done by all forces acting on an object is equal to the change in its kinetic energy