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Sophie [7]
3 years ago
10

A balky cow is leaving the barn as you try harder and harder to push her back in. In coordinates with the origin at the barn doo

r, the cow walks from x = 0 to x = 6.9 m as you apply a force with x-component F _ { x } = - [ 20.0 N + ( 3.0 N / m ) x ]F x =−[20.0N+(3.0N/m)x]. How much work does the force you apply do on the cow during this displacement?
Physics
1 answer:
Tresset [83]3 years ago
7 0

Answer:

The work done is -209.42 J.

Explanation:

F(x) = (- 20 - 3 x ) N

x = 0 to x = 6.9 m

Here, the force is variable in nature, so the work done by the variable force is given by

W =\int F dx\\\\W =\int_{0}^{6.9}(-20- 3x dx )\\\\W= \left [ - 20 x - 1.5 x^2 \right ]_{0}^{6.9}\\\\W = - 20 (6.9 - 0) - 1.5(6.9\times 6.9 - 0)\\\\W =- 138 - 71.42\\\\W = - 209.42  J

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(a) t=\frac{v}{a_1}+\frac{v}{a_2}

In the first part of the motion, the car accelerates at rate a_1, so the final velocity after a time t is:

v = u +a_1t

Since it starts from rest,

u = 0

So the previous equation is

v= a_1 t

So the time taken for this part of the motion is

t_1=\frac{v}{a_1} (1)

In the second part of the motion, the car decelerates at rate a_2, until it reaches a final velocity of v2 = 0. The equation for the velocity is now

v_2 = v - a_2 t

where v is the final velocity of the first part of the motion.

Re-arranging the equation,

t_2=\frac{v}{a_2} (2)

So the total time taken for the trip is

t=\frac{v}{a_1}+\frac{v}{a_2}

(b) d=\frac{v^2}{2a_1}+\frac{v^2}{2a_2}

In the first part of the motion, the distance travelled by the car is

d_1 = u t_1 + \frac{1}{2}a_1 t_1^2

Substituting u = 0 and t_1=\frac{v}{a_1} (1), we find

d_1 = \frac{1}{2}a_1 \frac{v^2}{a_1^2} = \frac{v^2}{2a_1}

In the second part of the motion, the distance travelled is

d_2 = v t_2 - \frac{1}{2}a_2 t_2^2

Substituting t_2=\frac{v}{a_2} (2), we find

d_1 = \frac{v^2}{a_2} - \frac{1}{2} \frac{v^2}{a_2} = \frac{v^2}{2a_2}

So the total distance travelled is

d= d_1 +d_2 = \frac{v^2}{2a_1}+\frac{v^2}{2a_2}

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3 years ago
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Explanation:

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8 0
3 years ago
A car of mass 1600 kg traveling at 27.0 m/s is at the foot of a hill that rises vertically 135 m after travelling a distance of
Zarrin [17]

Answer:

Neglecting any frictional losses, the average power delivered by the car's engine is 10565 W

Explanation:

The energy conservation law indicates that the energy must be the same at the bottom of the hill and at the top of the hill.  

The energy at the bottom is only the Kinect energy (K_1) of the car in motion, but in the top, the energy is the sum of its Kinect energy (K_2), potential energy (P) and the work (W) done by the engine.

K_1 = K_2 + P + W

then, the work done by the engine is:

W = K_1 - K_2 - P

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K=\frac{1}{2}mV^2\\P=mgh

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Using the formulas:

W=\frac{1}{2}mV_1^2-\frac{1}{2}mV_2^2-mgh

Replacing the values:

W=\frac{1}{2}(1600Kg)(27m/s)^2-\frac{1}{2}(1600Kg)(14m/s)^2-(1600Kg)(9.8m/s^2)(135m)\\W=-1690400 J

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The average speed of the car is (27+14)/2=20m/s, and t=d/v so the time is:

t=\frac{3200m}{20m/s}=160s

the power delivered by the car's engine was:

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h is the height (position) of the ball respect to a given point

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