An object with a mass of #1 kg# is pushed along a linear path with a kinetic friction coefficient of #u_k(x)= e^x-x+3 #. How much work would it take to move the object over #x in [1, 2], where x is in meters?
The work done is
We need
The frictional force is The normal force is So, But, The work done is
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To calculate the work done to move the object over the interval [1, 2], we need to integrate the force of kinetic friction over that interval. The force of kinetic friction ( F_k ) is given by the equation:
[ F_k = \mu_k \cdot N ]
where ( \mu_k ) is the kinetic friction coefficient and ( N ) is the normal force. Since the object is being pushed along a linear path, the normal force is equal to the weight of the object, which is ( mg ), where ( m ) is the mass of the object and ( g ) is the acceleration due to gravity.
The work done ( W ) is then given by the equation:
[ W = \int_{1}^{2} F_k , dx ]
Substituting ( F_k = \mu_k(x) \cdot mg ) into the equation, we get:
[ W = \int_{1}^{2} \left( e^x - x + 3 \right) \cdot mg , dx ]
Given that the mass of the object is ( m = 1 , \text{kg} ), and ( g = 9.8 , \text{m/s}^2 ), we can compute the integral:
[ W = \int_{1}^{2} \left( e^x - x + 3 \right) \cdot 1 \cdot 9.8 , dx ]
[ W = \left[ 9.8 \cdot \left( e^x - \frac{x^2}{2} + 3x \right) \right]_{1}^{2} ]
[ W = \left[ 9.8 \cdot \left( e^2 - \frac{2^2}{2} + 3 \cdot 2 - e - \frac{1^2}{2} + 3 \cdot 1 \right) \right] ]
[ W = 9.8 \cdot \left( e^2 - 2 + 6 - e - \frac{1}{2} + 3 \right) ]
[ W = 9.8 \cdot \left( e^2 - e + \frac{11}{2} \right) ]
[ W \approx 9.8 \cdot \left( 7.389 - 2.718 + 5.5 \right) ]
[ W \approx 9.8 \cdot 10.171 ]
[ W \approx 99.84 , \text{Joules} ]
Therefore, it would take approximately ( 99.84 , \text{Joules} ) of work to move the object over the interval [1, 2] meters.
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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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