work energy theorem explanation
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Workdone Under a Constant Force
We have already learnt about the equations of motion earlier and know that,
Here, v is the final velocity of the object; u is the initial velocity of the object; a is the constant acceleration and s is the distance traversed by the object. We can also write this equation as,
We can substitute the values in the equation with the vector quantities, therefore:
If we multiply both sides with m/2, we get:
From Newton’s second law, we know that F=ma, hence:
Now, we already know that W= F.d and, K.E. = (mv²)/2,
So, the above equation may be rewritten as:
Hence, we have:
Therefore, we have proved the Work-Energy Theorem. The Work done on an object is equal to the change in its kinetic energy.
We have already learnt about the equations of motion earlier and know that,
Here, v is the final velocity of the object; u is the initial velocity of the object; a is the constant acceleration and s is the distance traversed by the object. We can also write this equation as,
We can substitute the values in the equation with the vector quantities, therefore:
If we multiply both sides with m/2, we get:
From Newton’s second law, we know that F=ma, hence:
Now, we already know that W= F.d and, K.E. = (mv²)/2,
So, the above equation may be rewritten as:
Hence, we have:
Therefore, we have proved the Work-Energy Theorem. The Work done on an object is equal to the change in its kinetic energy.
pickachupradhan:
thnx for answer my ouestionn
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