How mush work is done in lifting a 40 kilogram weight to a height of 1.5 meters?

Answer 1
The answer is #588J#.

Always start with the definition:

#W=int_a^b F(x)dx#
Sometimes, the simple problems are the hardest because it looks too easy so we tend to add unnecessary things. Since this is a vertical lift, we are dealing with gravity which is 9.8 #m/s^2#. So,
#F(x)=9.8m/(s^2)*40kg=392N#
Remember that work is force times distance. We have force which is just a constant function. And we have distance which is #dx#. The tendency is to add an #x# into #F(x)=392N#, but that would be incorrect. Now, let's put it together:
#a=0# #b=1.5# #W=int_0^(1.5) 392 dx# #=392x|_0^(1.5)# #=588J#
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Answer 2

The work done in lifting a 40-kilogram weight to a height of 1.5 meters can be calculated using the formula for work:

[ \text{Work} = \text{Force} \times \text{Distance} \times \cos(\theta) ]

Where:

  • Force is the force exerted to lift the weight, which is equal to the weight of the object in this case.
  • Distance is the height through which the object is lifted.
  • θ is the angle between the force vector and the direction of motion. Since the force and the direction of motion are in the same line, θ = 0 and cos(θ) = 1.

Given:

  • Mass (m) = 40 kilograms
  • Height (h) = 1.5 meters
  • Acceleration due to gravity (g) ≈ 9.8 m/s² (assuming Earth's surface)

We can calculate the force exerted to lift the weight using Newton's second law:

[ \text{Force} = \text{Mass} \times \text{Acceleration due to gravity} ]

[ \text{Force} = 40 \times 9.8 ]

Now, calculate the work done:

[ \text{Work} = \text{Force} \times \text{Distance} \times \cos(\theta) ]

[ \text{Work} = (40 \times 9.8) \times 1.5 \times 1 ]

[ \text{Work} = 588 \text{ joules} ]

Therefore, the work done in lifting a 40-kilogram weight to a height of 1.5 meters is 588 joules.

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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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