physics as unit2 05 hookeslaw01
TRANSCRIPT
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1. To understand what happens when anincreasing force is applied to a wire or spring
2. To understand how springs in series and
parallel behave
3. To understand how to calculate the energy
stored in a stretched spring
4. Use this as a vehicle to check graph plotting
Book Reference : Pages 164-166
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http://www.rdg.ac.uk/acadepts/sp/picetl/publish/ISEs/Forces2.htm
What happens when you apply increasing
tension to a spring or wire?
Hookes Law states
that...the change in
length produced by a
force on a wire orspring is directly
proportional to the
force applied.
http://www.rdg.ac.uk/acadepts/sp/picetl/publish/ISEs/Forces2.htmhttp://www.rdg.ac.uk/acadepts/sp/picetl/publish/ISEs/Forces2.htm -
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Extension Force Applied
L F
Well see
latter that
Hookes law
only applieswithin limits
L (m)
F
(N
)
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To turn a proportionality into an equation
we need to introduce a constant ofproportionality...
L F
F = kL
We call k the spring constant and it defines
how stiff the spring is
How can we find K experimentally?
What should we do to minimise errors?
Take care to avoid confusion
between overall length &extension
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Take the
gradient ofthe graph :
F2F1L2L1
F
L
L (m)
1. Make the gradient triangle as large as possible
2. Avoid outliers, choose data points which are on
the line
F
(N)
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L (m)
When we undertake an experiment
we should only change one variable at
a time to make it a fair test. We call
this the independent variable
Quantities we measure, (and subsequently calculate) are
called dependent variables. All other variables which
are kept the same are called the control variables
Often graphs have the independent variable along
the bottom and the dependent up the side
Hookes law is a notable exception
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C stops obeying Hookes law... After the limit of
proportionality the material behaves in a ductile
fashion. The material stretches more with a
small extra force.
Spring constant :
material A isstiffer than B & C
L (m)
F
(N)
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Springs in parallel share the load &
have the same extension acting like a
single spring with a combined spring
constant
The force needed to stretch
springs p & q respectively is:-
Fp= kpL & Fq= kqL
Weight supported by both
springs W = Fp + Fq
p q
L
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Cancel out L
k = kp+ kq
p q
L
So by substituting & expanding
W = kpL + kqL which can be
considered equal to kL where
k is the effective spring
constant
kL = kpL + kqL
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Springs in series share the same
tension which is equal to W
The extensions in the two
springs is given by:-
Lp= W/kp& Lq= W/kq
The total extension is Lp+ Lq
W/k = W/kp+ W/kq = 1/kp+ 1/kq = 1/k
where k is the effective spring constant
p
qL
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The stretched spring
has elastic potentialenergy. Work has been
done because the
force moves through adistance.
The distance moved by the force is L, the
force involved ranges from 0 to F and so the
average is F/2
Ep= FL
Only valid for
where Hookes
law is obeyed
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1. Weve seen Hookes law and how we can useit to establish the spring constant
2. Weve discussed variables and how to
accurately establish the spring constantexperimentally
3. Weve seen how combinations of springs in
parallel and series can act as a single spring
4. We have related the elastic potential energy
in a stretched spring to the work done
stretching the spring