If the length of a #24 cm# spring increases to #47 cm# when a #5 kg# weight is hanging from it, what is the spring's constant?

Answer 1

Better to rewrite the question in metres: "#0.24 m# spring increases #0.47 m#..." Spring constant, #k = F/(Delta d) = (m*g)/(Delta d) = (5*9.8)/(0.47-0.24) = 21.3 Nm^-1#

The spring constant, #k#, of a spring is expressed in newton per metre #(Nm^-1)#: for each additional #N# of force the spring expands by #k (m)#.
It's important to use correct SI units for the quantities: centimetre is not a base SI unit, metre is, so convert the #cm# to #m#.
I used #Delta d# to represent the change in length of the spring - final length of #0.47 m# minus initial length #0.24 m#.
The force acting on the spring is the weight force of the mass, which is its mass, #5 kg# times #g = 9.8 Nkg^-1# (more often written as #ms^-2#, but this is an exactly equivalent unit that makes more sense in this context).
Calculating all this leads to a spring constant equal to #21.3 Nm^-1#.
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Answer 2

The spring constant, ( k ), can be calculated using Hooke's Law:

[ F = -kx ]

Where:

  • ( F ) is the force applied to the spring (weight of the object),
  • ( k ) is the spring constant,
  • ( x ) is the displacement from the equilibrium position.

Given:

  • ( F = mg ) (weight of the object),
  • ( m = 5 ) kg,
  • ( g = 9.8 ) m/s(^2) (acceleration due to gravity),
  • Initial length (( x_1 )) = 24 cm = 0.24 m,
  • Final length (( x_2 )) = 47 cm = 0.47 m.

Using Hooke's Law:

[ F = k(x_2 - x_1) ]

[ mg = k(x_2 - x_1) ]

[ k = \frac{mg}{x_2 - x_1} ]

[ k = \frac{5 \times 9.8}{0.47 - 0.24} ]

[ k ≈ \frac{49}{0.23} ]

[ k ≈ 213.04 , \text{N/m} ]

So, the spring constant is approximately ( 213.04 , \text{N/m} ).

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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