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Question: Show that the sum of kinetic energy and potential energy (i.e., total mechanical energy) is always c...

Show that the sum of kinetic energy and potential energy (i.e., total mechanical energy) is always conserved in the case of a freely falling body under gravity (with air resistance neglected) from a height h by finding it when
(i) the body is at the top,
(ii) the body has fallen a distance xx,
(iii) the body has reached the ground.

Explanation

Solution

Calculate the kinetic and potential energy at each of the instances asked in the question. The sum of potential and kinetic energy gives the total mechanical energy of the system. Since we have ignored the force of friction, we don’t need to worry about the loss of energy due to friction (energy remains conserved for this system)

Formulas used:
v2=u2+2as{v^2} = {u^2} + 2as
Where vv is the initial velocity, uu is the final velocity, aa is the acceleration and ss is the distance covered.
U=mghU = mgh
Where, UU is the total potential energy, mm is the mass of the object, gg is the acceleration due to gravity and hh is the height of the object from the ground
K=12mv2K = \dfrac{1}{2}m{v^2}
Where, KK is the total kinetic energy, mm is the mass of the object and vv is the velocity of the object at that moment.

Complete step by step answer:
So, in the given diagram a body of mass m be falling freely under gravity from a height h above the ground (i.e., from position ‘a’). Let us now calculate the sum of kinetic energy K and potential energy U at various positions, say at ‘a’ (at height h above the ground), at ‘b’ (when it has fallen through a distance x) and at ‘c’ (on the ground).

(i) At the position ‘a’ (at height h above the ground):
The initial velocity of body= 0 (since body is at rest at A)
Kinetic energy =12×m×(0)2=0 = \dfrac{1}{2} \times m \times {\left( 0 \right)^2} = 0
Potential energy U=mghU = mgh
Hence total mechanical energy =0+mgh=mgh = 0 + mgh = mgh...........(I)

(ii) At the position ‘b’ (when it has fallen a distance x): Let vx{v_x} be the velocity acquired by the body at ‘b’ after falling through a distance x. Then the values initial velocity (u=0)\left( {u = 0} \right),distance (S=x)\left( {S = x} \right) and acceleration (a=g)\left( {a = g} \right). From the above equation v2=u2+2as{v^2} = {u^2} + 2as. The value of vx{v_x} is:
vx2=02+2gx{v_x}^2 = {0^2} + 2gx (Substituting all the values)
vx=2gx\Rightarrow {v_x} = 2gx
Hence, Kinetic energy

\Rightarrow K= \dfrac{1}{2}m \times 2gx \\\ \Rightarrow K = mgx$$ Now at the point ‘b’, height of body above the ground $ = h - x$. Potential energy is, $$U = mg\left( {h{\text{ }}-{\text{ }}x} \right)$$ The total mechanical energy is $$T= K + U \\\ \Rightarrow T = mgx + mg\left( {h{\text{ }}-{\text{ }}x} \right) \\\ \Rightarrow T = mgh$$.............(II) (iii) At the position ‘c’ (on the ground): Let the velocity acquired by the body on reaching the ground be ${v_g}$. Then the values initial velocity $\left( {u = 0} \right)$, distance $\left( {S = h} \right)$ and acceleration $\left( {a = g} \right)$. From the above equation${v^2} = {u^2} + 2as$. ${v_g}^2 = {0^2} + 2gh$ (Substituting all the values) $\Rightarrow {v_g} = 2gh$ So, kinetic energy is, $$K = \dfrac{1}{2}m{v_g}^2 \\\ \Rightarrow K= \dfrac{1}{2}m \times \left( {2gh} \right) \\\ \Rightarrow K= mgh$$ Potential energy $$U = mg \times 0 = 0$$ (at the ground when h = 0) The total mechanical energy $$ = K + U = mgh + 0 = mgh$$...............(III) It is completely clear from equation (I), (II) and (III), we get to see that the total mechanical energy which is the sum of kinetic energy and potential energy always remains constant at each point of motion and is equal to initial energy at height $h$. **Note:** If friction is ignored the above is valid, but if friction is encountered the total mechanical energy decreases as the height decreases and the energy doesn’t remain conserved. In some questions the height to which the object is thrown is given to be very large (in terms comparable to the radius of earth) in such cases the value of acceleration due to gravity $\left( g \right)$ changes. In such cases we use to $\left( {U = - \dfrac{{GMm}}{X}} \right)$ calculate the potential energy of the object where $M$ is the mass of earth, $m$ is the mass of the object, $G$ is the gravitational constant and $X$ is the distance of the object from the centre of the earth.