Materials Flashcards
How to find density of a regular solid?
(how to reduce uncertainty?)
Measure mass using top pan balance.
Measure dimensions using Vernier caliper or micrometer and calculate volume using appropriate eq.
Calculate density, ρ = m / v
Density of liquid?
(how to reduce uncertainty?)
Mass of empty cylinder. Add liquid (use as much liquid as possible to reduce % error). Mass of cylinder + liquid. Volume of liquid in cylinder. Calculate density.
Density of irregular solid?
Measure mass. Immerse in liquid in measuring cylinder and observe rise in liquid level. This is volume. Calculate density.
Density of alloys?
Mass of alloy, m = ρAVA + ρBVB
Density of alloy, ρ = m/v
= (ρAVA + ρBVB) / V
= ρAVA / V + ρBVB / V
1 m^3 into cm^3?
10^6 cm^3
What is the tension in a spring (describe) ?
A stretched spring exerts a pull on the object holding each end of the spring. This pull, referred to as the tension in the string, is equal and opposite to the force needed to stretch the spring.
What is Hooke’s law?
States that the force needed to stretch a spring is directly proportional to the extension of the string from its natural length, UP to a limit of proportionality. F = k ΔL
What is k?
k is spring constant/stiffness constant. the greater the value of k the stiffer the spring.
Springs in parallel:
k = k1+ k2
(same ΔL)
Springs in series:
1/k = 1/k1 + 1/k2
(same F)
Elastic potential energy is stored in a stretched spring. What’s the eq?
Ep = 1/2 F ΔL = 1/2 k ΔL^2
What is elasticity?
Elasticity of a solid material is its ability to regain its shape after it has been deformed or distorted and the force that deformed it has been released.
Deformation that stretches an object is …
..tensile.
Deformation that compresses an object is…
..compressive.
How to test how easily different materials stretch?
(experiment) (graph axes)
Add weights, measure, using a set square and metre ruler, ΔL from L0 each time, then unload until no weights.
ΔL(y) against T (x)
Steel spring ΔL-T graph:
Straight line through origin because of Hooke’s law.
Rubber band ΔL-T graph:
Rubber band extends easily when it’s stretched. However, becomes fully stretched and very difficult to stretch further when its been lengthened considerably.
got an acceleration start curving up then at end curves towards other direction so s shaped. at all points its below the spring line.
Polythene string ΔL-T graph:
Polythene string ‘gives’ and stretches easily after its initial stiffness is overcome. However, after ‘giving’ easily, it extends little and becomes difficult to stretch.
got a very shallow start then curves up steeply and changes direction at end. at all points its below the spring line and the rubber band line.
How can we measure extension of a wire under tension ?
Using Searle’s apparatus.
Micrometer attached to control wire adjusted so the spirit level between the control and test wire is horizontal. Each time weight added, micrometer readjusted. Readjustments are the ΔL.
For a wire under tension, tensile stress is?
Units?
Tensile stress = tension per unit cross-sectional area.
σ = T / A
Units Pa or Nm^-2
For a wire under tension, tensile strain is?
Units?
Tensile strain = extension per unit length.
ε = ΔL / L0
No units bc its a ratio.
We have a stress-strain graph. Try drawing it, inc limit of proportionality, elastic limit, yield point 1 and 2, plastic flow, UTS, and breaking point.
First directly proportional. Instant it stops being directly proportional is P (limit of proportionality). Just beyond it we have E (elastic limit) then a peak of this mini n shape called Y1 and the bottom of this n shape called Y2. Kind of looks like a walking stick at an angle rn. From here extends at an angle to the right, reaching a shallow peak (UTS) and curving down to a stop at B (breaking point).
From 0 to limit of proportionality, P, stress ∝ strain. Gradient is Young modulus, E:
E = σ/ε = T L0 / ΔL A
Beyond P line curves and continues beyond elastic limit, E, to yield point Y1, which is:
which is where the wire weakens temporarily.