- Work done Formula
- Work done by variable force
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- Kinetic energy
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- Work Energy theorem
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- Potential energy
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- Potential energy of the spring
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- Conservative Forces
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- Mechanical Energy and Conservation
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- Power definition
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- Law of Conservation of energy
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- Work Energy and Power Solved Examples

- So far we have defined work done by a force which is constant in both magnitude and direction.

- However, work can be done by forces that varies in magnitude and direction during the displacement of the body on which it acts.

- For simplicity consider the direction of force acting on the body to be along x-axis also consider the force F(x) is some known function of position x

- Now total displacement or path of the body can be decomposed into number of small intervals Δx such that with in each interval force F(x) can be considered to be approximately constant as shown below in the figure

- Work done in moving the body from x
_{1}to x_{2}is given by

ΔW=F(x_{1})Δx_{1}where Δx_{1}=x_{2}-x_{1}

- Total work done in moving the body from point A to point B

W=F(x_{1})Δx_{1}+F(x_{2})Δx_{2}+F(x_{3})Δx_{3}.....+F(x_{n})Δx_{n}

W=Σ F(x_{i})Δx_{i}where i=1 to i=n (4)

Where Σ is the symbol of summation

- Summation in equation 4 is equal to shaded area in figure 3(a) .More accuracy of results can be obtained by making these interval infinitesimally smaller

- We get the exact value of work done by making each interval so much small such that #916;x-> 0 which means curved path being decomposed into infinite number of line segment i.e

W= Lim_{Δx-> 0}Σ F(x_{i})Δx_{i}(5)

$W= \int_{x_a}^{x_b} fdx$ Where $\int_{x_a}^{x_b} fdx$ is the integral of F(x) w.r.t x between the limits x_{A}and x_{B}and integral can be evaluated using methods of calculus if F(x) of x is known

- Instead of x if the force also acts along y and z axis i.e direction of force keeps on changing then work done by such a force is given by

W=∫ F(**r**)d**r**with in the limits**r**and_{A}**r**(6)_{B}

Where F(**r**)=F(x)**i**+F(y)**j**+ F(z)**k**

and d**r**=dx**i**+dy**j**+ dz**k**

Here F(x),F(y) and F(z) are rectangular components of the force along x ,y and z axis .Similarly dx,dy and dz are rectangular components of displacement along

x ,y and z axis

- Work done by the variable force along x-axis can also be calculated using the graphical way also. The area enclosed by the Force displacement gives the work done by the variable force

A object of mass m= 2 kg is subjected by the variable force in x-direction. The force varies as per the below function

$F_x= (3 + .2 x) N$

Find the work done by the force in moving the object from x=0 to x= 5 m?

$W= \int_{x_a}^{x_b} fdx$

$W= \int_{0}^{5} (3 + .2x) dx = 17.5 J $

A particle is acted by the force along x-axis which varies as given in below graph

a. Find the work done from x=0 to x=5 m

b. Find the work done from x=5 to x=10 m

c. Find the work done from x=10 to x=15 m

Work done by will given by the area enclosed

a. work done from x=0 to x=5 m = $ \frac {1}{2} \times 300 \times 5 = 750 N$

b. work done from x=5 to x=10 m = $ 300 \times 5 = 1500 N$

c. work done from x=10 to x=15 m = $ \frac {1}{2} \times 300 \times 5 = 750 N$

b. Calculate the work done by the force applied by Man over 20 m.

c. Calculate the work done by the frictional force over 20 m.

d. Calculate the net work done on trunk

The plot of the force applied by the man (F) and Frictional force (50 N) is given below

The frictional force is constant and acts in the opposite direction to the applied force.So it is shown as negative in the graph

Now The work done by the man is given by the area enclosed by the Force F in the above graph

Work done= area of the rectangle + area of the trapezium

$W= 100 \times 10 + \frac {1}{2} (100 + 50 ) \times 10$

= 1000 + 750

= 1750 J

Now The work done by the frictional force is given by the area enclosed by the friction force (-50 N) in the above graph

Work done= area of the rectangle

$ W = -50 \times 20 = -1000 J $

Net work done= 1750 -1000 = 750 J

Class 11 Maths Class 11 Physics Class 11 Chemistry

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