Understanding the Force Constants of Springs in Combination

AI Thread Summary
Calculating the force constants of springs in combination involves understanding their configurations. In parallel, the total spring constant is the sum of individual constants, as the extension remains the same. In series, the total spring constant is found by taking the inverse of the sum of the inverses of the individual constants, as the total extension is the sum of the extensions of each spring. The mass does not affect the spring constants directly; only the configuration matters. Proper application of these principles allows for accurate calculations of combined spring constants.
emilykay
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I don't understand how to calculate force constants of a combination of springs.

for example 2 spings parallel with the mass on one end lying on a table.

or 2 springs attached with mass at one end lying on a table.

i know that force constant = sum of forces/ extension
but just don't get how to combine springs!

Thanks!

EmilyKay
 
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Hey Its Easy Man.just Assume The Springs As Resistance And Like We Calculate Net Resistances In Series And In Parallel Calculate The Net Spring Constant.ex-two Springs Of Spring Constant =k Conected In Series Are Equal Ti A Spring Of Constant 2k.the Masses Have Got No Role To Play.only Thing Is That U Have To Find How They Aye Joined In Seriesa Or Parallel.ok...
 
when in Parallel configurations:
since they are parallel, the extension must be the same.
k=sum (F) / x
hence k=(F_1+F_2)/x = k_1+k_2

when in series configurations:
when in equilibrium, the tension in the two springs must be equal and the extension is the extension of the first spring + the extension of the second spring:
k=F/ (x1+x2)
take the inverse of both side:
\frac{1}{k}=\frac{x_1}{F}+\frac{x_2}{F}=\frac{1}{k_1}+\frac{1}{k_2}
 
rohit88 response is incorrect. Please pay attention to the response given by tim_lou, which is the correct answer AND derivation.

Springs in series behave like resistors in parallel, which springs in parallel behave like resistors in series.

Zz.
 
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