Materials

Density

The density of a substance is defined as the mass per unit volume. It can be calculated using the formula:

$$ \rho = \frac{m}{V} $$

Where $\rho$ is the density measured in $kgm^{-3}$, $m$ is the mass measured in $kg$, and $V$ is the volume measured in $m^{3}$.

An unknown substance can be identified if its density is measured and compared to the density of known substances. c

Density of alloys

An alloy is a solid mixture of two or more metals. The density of the alloy can be found by dividing the mass of both metals by the volume.
$$ \rho = \frac {\rho_{A}V_{A} + \rho_{B}V_{B}}{V} $$

Hooke's Law

Hooke's Law states that the force needed to stretch a spring is directly proportional to the extension of the spring from its natural length. Hooke's Law may be written as:

$$ F = k \Delta L $$

Where $k$ is the spring constant, and $\Delta L $ is the extension. The greater the value of $k$, the greater the force required to stretch the spring. If a spring is stretched beyond its elastic limit, it is unable to regain its original length.

Springs in Parallel

As the weight is supported by both of the springs, the weight:
$$ W = F_{P} + F_{Q} = k_{P}\Delta L + k_{Q}\Delta L $$
With the effective spring constant as:
$$ k = k_{P} + k_{Q} $$

hookes-parallel

Springs in series

For springs in parallel, the extension of the springs is not equal, although the tension in each spring is the same. This means that the total extension is:

$$ \Delta L = \Delta L_{P} + \Delta L_{Q} = \frac {W}{k_{P}} + \frac {W}{k_{P}} $$

The effective spring constant is:
$$ \frac {1}{k} = \frac {1}{k_{P}} + \frac {1}{k_{Q}} $$

hookes-series

Energy stored in a stretched spring

Elastic potential energy is stored in a stretched spring. If the spring is released, the elastic potential energy is suddenly converted into kinetic energy. The elastic potential energy can be calculated by:

$$ E_{P} = \frac{1}{2}F \Delta L = \frac{1}{2}k \Delta L^{2} $$

Deformation of solids

The elasticity of a material is its ability to regain it's shape after been stretched. Deformation that stretches an object is tensile while deformation that compresses an object is compressive.

Stress

Tensile stress is a measure of the force per unit area of a material.
$$ \sigma = \frac{T}{A} $$
Where $\sigma$ is the stress measured in $Nm^{-2}$, $T$ is the tension and $A$ is the cross sectional area.

Strain

Tensile strain is defined as the extension per unit length.
$$ \epsilon = \frac{\Delta L}{L} $$
Where $\epsilon$ is the strain with no units as it is a ratio. Both $\Delta L$ and $L$ must use the same units.

Stress and Strain of a wire

Below is a graph showing the stress against strain for a wire.

stress-strain-points

Between the origin and the limit of proportionality P, the strain is proportional to the stress. This means that at this stage, it has a constant Young modulus.

$$ \text{Young modulus} = \frac {\sigma}{\epsilon} $$

Once it passes the elastic limit, the point of which the wire is permanently stretched, and reaches the yield point $Y_{1}$, it weakens temporarily. Beyond $Y_{2}$, plastic flow occurs before reaching the ultimate tensile stress where the wire starts to become thinner and break.

Stress-strain curve

The stiffness can be determined by calculating the gradient of a stress-strain line which is the Youngs Modulus. The greater Youngs Modulus is, the stiffer the material is.

stress-strain

Loading and Unloading

load-wire

load-rubber

The area below the loading curve is the work done to stretch the band. The area below the unloading curve is the work done when it is unloaded. The area between the lines is the energy stored as internal energy in the molecules.

load-polythene

The area between the loading the unloading curves represent the work done to deform the material permanently.

© Andrew Deniszczyc, 2018