weights attached to a spring. The more weights = the bigger the extension
when plotted, we can see a line going through origin and directly proportional of f and x
Hooke’s Law = the extension is proportional to the force applied, providing the limit of proportionally has not been breached
F = kx
Springs in parallel and series (not in spec but comes up in exams):
When in parallel:
1/2 extension for the same force so higher spring constant
spring constant = k1 + k2
When in series:
both springs extend and experience same force so extension = 2x
spring constant (lower) = 1/kt = 1/k1 + 1/k2
Basically just the opposite of resistors
Elastic potential energy in springs:
areaunder f x graph = elastic potential energy stored
area = 1/2 fx
area = 1/2(kx)x
Stress, strain and young’s modulus:
Stress = force / area (nm^-2)
Strain = extension / original length (no units)
stress / strain = young‘s modulus
Stress-strain graph:
Limit of proportionality = any further young’smodulus won’t be true
elastic limit = if load is retracted, the material will still return to its original form
yield point = so much stress causes lots of strain. (like blue tack when you hardly pull it yet it extends a lot)
ultimate tensile strength - failure occurs here
Ductile and brittle materials:
Brittle materials tolerate a lot of stress and don’t have much strain. Have a higher gradient. Have a higher UTS (ultimate tensile strength) (crunchie)
Ductile materials are most metals - has a lower yield point and a long period of increased strain. (Mars)
Polymers have a much lower elastic limit and yield point - massive amount of strain accepted. (Lowest gradient)
Behaviour of rubber:
a plotted stress strain graph of rubber creates a hysteresis loop
the area inside the loop is the energy transferred per unit volume
it doesn’t obey hooke’s law so stress is not directly proportional to strain
With cars, they undergo a lot of compression and extension whilst driving. This causes the tyres to heat up