$${\text{Mechanical efficiency}} = \frac{{{\text{Output work }}}}{{{\text{Input work}}}}$$
The output work will increase because the friction becomes less. Thus the mechanical efficiency increases.
2.
A force acts on a $$30\,gm$$ particle in such a way that the position of the particle as a function of time is given by $$x = 3t - 4{t^2} + {t^3},$$ where $$x$$ is in metres and $$t$$ is in seconds. The work done during the first $$4$$ seconds is
3.
Two equal masses $${m_1}$$ and $${m_2}$$ moving along the same straight line with velocities $$+ 3\,m/s$$ and $$- 5\,m/s$$ respectively collide elastically. Their velocities after the collision will be respectively
Given, $${u_1} = 3m/s,\,{u_2} = - 5\,m/s,\,{m_1} = {m_2} = m$$
According to principle of conservation of linear momentum,
$$\eqalign{
& {m_1}{u_1} + {m_2}{u_2} = {m_1}{v_1} + {m_2}{v_2} \cr
& m \times 3 - m \times 5 = m{v_1} + m{v_2} \cr} $$
$${\text{or}}\,\,{v_1} + {v_2} = - 2\,.....\left( {\text{i}} \right)$$
In an elastic collision, $$e = \frac{{{v_2} - {v_1}}}{{{u_1} - {u_2}}}$$
$$\eqalign{
& \Rightarrow {v_2} - {v_1} = e\left( {{u_1} - {u_2}} \right) \cr
& \Rightarrow {v_2} - {v_1} = \left( 1 \right)\left( {3 + 5} \right)\,\,\left( {\because e = 1} \right) \cr
& \Rightarrow {v_1} - {v_2} = - 8\,......\left( {\text{ii}} \right) \cr} $$
Adding Eqs. (i) and (ii), we obtain
$$\eqalign{
& 2{v_1} = - 10 \cr
& \Rightarrow {v_1} = - 5\,m/s \cr} $$
From Eq. (i), $${v_2} = - 2 - {v_1} = - 2 + 5 = 3\,m/s$$
Thus, $${v_1} = - 5\,m/s,\,{v_2} = + 3\,m/s$$
If two bodies collide elastically, then their velocities are interchanged. Since, it is an elastic collision hence, velocities after collision will be $$-5\,m/s$$ and $$3\,m/s.$$
4.
A variable force $$P$$ is maintained tangent to a frictionless cylindrical surface of radius $$a$$ as shown in figure. By slowly varying this force, a block of weight $$W$$ is moved and the spring to which it is stretched from position $$1$$ to position $$2.$$ The work done by the force $$P$$ is
A.
$$W\,a\sin \theta $$
B.
$$\frac{1}{2}k{a^2}{\theta ^2}$$
C.
$$W\,a\sin \theta + k{a^2}{\theta ^2}$$
D.
$$W\,a\sin \theta + \frac{1}{2}k{a^2}{\theta ^2}$$
5.
A force applied by an engine of a train of mass $$2.05 \times {10^6}kg$$ changes its velocity from $$5\,m/s$$ to $$25\,m/s$$ in $$5$$ minutes. The power of the engine is
6.
A $$1\,kg$$ particle at a height of $$8\,m$$ has a speed of $$10\,m/s$$ down a fixed incline making an angle $${53^ \circ }$$ with horizontal as shown in figure. It slides on a horizontal section of length $$10\,m$$ at ground level and then up a fixed incline making an angle $${37^ \circ }$$ with horizontal. All surfaces have $${\mu _k} = 0.5.$$ How far (in meters) from point $$O$$ (bottom of right inclined plane), along the incline making an angle $${37^ \circ }$$ with horizontal, does the particle first come to rest ?
Let $$x$$ be the distance travelled by the particle along the $${37^ \circ }$$ incline, after which it comes to rest. From work-energy theorem, Work done by gravity on block on incline $${53^ \circ } + $$ work done by friction on block on incline $${53^ \circ } + $$ work done by friction on ground level $$+$$ work done by gravity on block on incline $${37^ \circ } + $$ work done by friction on block on incline $${37^ \circ } = $$ change in $$K.E.$$ $$mg\left( 8 \right) - \mu mg\cos {53^ \circ }\left( {10} \right) - \mu mg\left( {10} \right) - \mu mg\cos {37^ \circ }\left( x \right) - mg\sin {37^ \circ }\left( x \right) = 0 - \frac{1}{2}\left( 1 \right){\left( {10} \right)^2}$$
On solving we get $$x = 1\,m$$
7.
A shell is fired from a cannon with a velocity $$v$$ $$\left( {m/\sec .} \right)$$ at an angle $$\theta $$ with the horizontal direction. At the highest point in its path it explodes into two pieces of equal mass. One of the pieces retraces its path to the cannon and the speed (in $$m/\sec.$$ ) of the other piece immediately after the explosion is
As one piece retraces its path, the speed of this piece just after explosion should be $$v\cos \theta $$
Applying conservation of linear momentum at the highest point;
$$\eqalign{
& m\left( {v\cos \theta } \right) = \frac{m}{2} \times v' - \frac{m}{2} \times v\cos \theta \cr
& 3v\cos \theta = v' \cr} $$
8.
A spring of force-constant $$k$$ is cut into two pieces such that one piece is double the length of the other. Then the long piece will have a force-constant of-
KEY CONCEPT
The force constant of a spring is inversely proportional to the length of the spring.
Let the original length of spring be $$L$$ and spring constant is $$k$$ (given)
Therefore,
$$\eqalign{
& k \times L = \frac{{2L}}{3} \times k' \cr
& \Rightarrow k' = \frac{3}{2}k \cr} $$
9.
How much water, a pump of $$2\,kW$$ can raise in one minute to a height of $$10\,m,$$ take $$g = 10\,m/{s^2}$$ ?
$$\eqalign{
& P = \frac{W}{t}.\,{\text{Here,}}\,P = 2\;kW = 2000\;W. \cr
& W = Mgh = M \times 10 \times 10 = 100M \cr
& {\text{and}}\,\,t = 60\,s. \cr} $$
This gives, $$M = 1200\,kg$$
Its volume = 1200 litre as 1 litre of water contains $$1\,kg$$ of its mass.
10.
An electric pump is used to fill an overhead tank of capacity $$9{m^3}$$ kept at a height of $$10\,m$$ above the ground. If the pump takes 5 minutes to fill the tank by consuming $$10\,kW$$ power the efficiency of the pump should be
$$\left( {g = 10\,m{s^{ - 2}}} \right)$$