An object with a mass of #7 kg# is pushed along a linear path with a kinetic friction coefficient of #u_k(x)= 4+secx #. How much work would it take to move the object over #x in [(-5pi)/12, (pi)/6], where x is in meters?
The work is
We require
The completed work is
The force of friction is
The completed work is
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To calculate the work done to move the object over the given interval, we need to integrate the force of friction with respect to distance. The force of kinetic friction ( F_k ) can be expressed as ( F_k = \mu_k \cdot N ), where ( \mu_k ) is the coefficient of kinetic friction and ( N ) is the normal force.
The normal force ( N ) can be calculated as ( N = mg ), where ( m ) is the mass of the object and ( g ) is the acceleration due to gravity.
Substituting the given values, we have ( N = (7 , \text{kg}) \cdot (9.8 , \text{m/s}^2) = 68.6 , \text{N} ).
Now, we need to integrate the force of friction over the given interval ( \left[ -\frac{5\pi}{12}, \frac{\pi}{6} \right] ):
[ W = \int_{-\frac{5\pi}{12}}^{\frac{\pi}{6}} F_k , dx ]
[ W = \int_{-\frac{5\pi}{12}}^{\frac{\pi}{6}} (4 + \sec(x)) \cdot (68.6) , dx ]
[ W = 68.6 \int_{-\frac{5\pi}{12}}^{\frac{\pi}{6}} (4 + \sec(x)) , dx ]
[ W = 68.6 \left[ 4x + \ln|\sec(x) + \tan(x)| \right]_{-\frac{5\pi}{12}}^{\frac{\pi}{6}} ]
[ W \approx 68.6 \left[ \frac{\pi}{3} - \frac{5\pi}{6} + \ln\left|\sec\left(\frac{\pi}{6}\right) + \tan\left(\frac{\pi}{6}\right)\right| - \left(-\frac{5\pi}{6} + \ln\left|\sec\left(-\frac{5\pi}{12}\right) + \tan\left(-\frac{5\pi}{12}\right)\right|\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} - \frac{5\pi}{6} + \ln\left|\sqrt{3} + 1\right| - \left(-\frac{5\pi}{6} + \ln\left|\sqrt{3} - 1\right|\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} - \frac{5\pi}{6} + \ln\left(\sqrt{3} + 1\right) + \frac{5\pi}{6} - \ln\left(\sqrt{3} - 1\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln\left(\sqrt{3} + 1\right) - \ln\left(\sqrt{3} - 1\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln\left(\frac{\sqrt{3} + 1}{\sqrt{3} - 1}\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln\left(\frac{(\sqrt{3} + 1)^2}{3 - 1}\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln\left(\frac{3 + 2\sqrt{3} + 1}{2}\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln\left(\frac{4 + 2\sqrt{3}}{2}\right) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + \ln(2 + \sqrt{3}) \right] ]
[ W \approx 68.6 \left[ \frac{\pi}{3} + 0.916 \right] ]
[ W \approx 68.6 \times 1.926 ]
[ \boxed{W \approx 132.159 , \text{J}} ]
So, it would take approximately 132.159 Joules of work to move the object over the given interval.
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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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