Chapter 6- Materials Flashcards

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1
Q

Within Hooke’s law region

A
F = kx 
Force = force constant x extension
N = Nm-1 x m
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2
Q

Past the elastic limit

A

Hooke’s law no longer applies (greater extension)

Plastically deformed as it doesn’t return to the same length when you let it go

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3
Q

Energy stored in spring

A

1/2 k x^2

Substitute Hooke’s law into the area under the curve (E = 1/2 Fx)

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4
Q

Springs in series

A

On top of each other

The inverse of the total force constant is the sum of the inverse of each

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5
Q

Springs in parallel

A

Alongside each other
The total force constant is the sum of each individual
The force applied to each is the total force divided by the number of springs

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6
Q

Brittle

A

Fails under load by cracking - little plastic deformation

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7
Q

Ductile

A

Can be drawn into wires and have a very large plastic region

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8
Q

Hysteresis Loop

A

An example is rubber
The area under the loading line is greater than the area under the unloading line
Still follows Hooke’s law
Shows energy is transferred to thermal (difference in areas under)

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9
Q

Work from force extension graph

A

Area under the loading curve

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10
Q

Energy stored from force extension graph

A

Area under unloading curve

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11
Q

Stress

A

The force per cross-section area

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12
Q

Stress equation

A
Stress = Force/Area
σ = F/A

Units Pa or Nm^-2

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13
Q

Strain

A

A measure of the relative change in length, the extension per unit length

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14
Q

Strain equation

A
Strain = extension/original length
ε = x/L

No units

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15
Q

Young’s Modulus

A
Stiffness = Stress/strain
E = σ/ε
E = F/A divided by x/L
E = FL/Ax

Units Pa/Nm^-2

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16
Q

Stress-strain vs force-extension graphs

A

Both have the same shape, stress-strain preferable as they depend on the properties of a material rather than the dimensions

17
Q

Stress-strain graph shape

A

Increase proportionally until the limit of proportionality, when strain is greater. Then it reaches the elastic limit in this section. It reaches a yield point where a large amount of plastic deformation (strain) happens without extra load. It flattens before increasing slightly to a peak (ultimate tensile strength) before decreasing as it breaks.

18
Q

Metal wire

A

Follows Hooke’s law until a fairly high elastic limit and then starts to curve
Unloading curve identical to loading before elastic limit
After the elastic limit, the unloading curve is parallel to the the Hooke’s law region all the way up

19
Q

Rubber

A

Loading curve starts with a high gradient before flattening and then rising again
Unloading curve broadly the same shape but lower
Does not follow Hooke’s law
When strain is the x-axis

20
Q

Polythene

A

Does not obey Hooke’s law, no elastic region
Loading curve similar to rubber but steeper earlier on
The unloading curve is a steep straight line not passing through the origin to represent plastic deformation

21
Q

Thermal energy wasted from a force extension graph

A

Area between the loading and unloading curves