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Which of the following is a one-dimensional motion?
(d) Motion of train on straight track is a one dimensional motion whereas everything else is a two dimensional or three dimensional activity.
A person moves towards east for \(3 \mathrm{~m}\), then towards north for \(4 \mathrm{~m}\) and then moves vertically up by \(5 \mathrm{~m}\). What is his distance now from the starting point?
Now, write the final position vector of the particle as follows.
\(
\vec{r}=3 \hat{i}+4 \hat{j}+5 \hat{k}
\)
The distance of the person from the origin is calculated by finding the magnitude of the position vector as,
\(
\begin{array}{l}
|\vec{r}|=\sqrt{3^2+4^2+5^2} \\
\Rightarrow \sqrt{9+16+25} \\
\Rightarrow 5 \sqrt{2}
\end{array}
\)
A particle moves in a circle of radius \(R\) from \(A\) to \(B\) as shown in figure. The distance covered by the object is
\(
\text { (a) Distance }=\text { Length } A B=2 \pi R \times \frac{60}{360}=\frac{\pi R}{3}
\)
A wheel of radius \(1 \mathrm{~m}\) rolls forward half a revolution on a horizontal ground. The magnitude of displacement of the point of the wheel initially in contact with the ground is
(c) Horizontal distance covered by the wheel in half revolution \(=\pi R\)
So, the displacement of the point which was initially in
\(
\begin{aligned}
\text { contact with ground } & =A A^{\prime}=\sqrt{(\pi R)^2+(2 R)^2} \\
& =R \sqrt{\pi^2+4}=\sqrt{\pi^2+4} \quad(\mathrm{As}, R=1 \mathrm{~m})
\end{aligned}
\)
The three initial and final position of a man on the \(X\)-axis are given as
(i) \((-8 \mathrm{~m}, 7 \mathrm{~m})\)
(ii) \((7 \mathrm{~m},-3 \mathrm{~m})\)
(iii) \((-7 \mathrm{~m}, 3 \mathrm{~m})\)
Which pair gives the negative displacement?
(i) The displacement of the man from \(A\) to \(E\) is \(\Delta x=x_2-x_1=7 \mathrm{~m}-(-8 \mathrm{~m})=+15 \mathrm{~m}\) directed in the positive \(x\)-direction.
(ii) The displacement of the man from \(E\) to \(C\) is \(\Delta x=-3 \mathrm{~m}-(7 \mathrm{~m})=-10 \mathrm{~m}\) directed in the negative \(x\)-direction.
(iii) The displacement of the man from \(B\) to \(D\) is \(\Delta x=3 \mathrm{~m}-(-7 \mathrm{~m})=+10 \mathrm{~m}\) directed in the positive \(x\)-direction.
The numerical ratio of displacement to the distance covered is always
(c) Since, displacement is always less than or equal to distance but never greater than distance. Hence, numerical ratio of displacement to the distance covered is always equal to or less than one.
A particle moves along a circular path of radius \(R\). The distance and displacement of a particle after one complete revolution is
\(
\begin{aligned}
\text { circumference of circle } & =2 \pi R \\
\text { distance } & =2 \pi R
\end{aligned}
\)
\(\Delta x=x_f – x_i\)
\(
x_f=x_i
\)
displacement \(=\Delta x=0\)
A particle starts from the origin, goes along \(X\)-axis to the point \((20 \mathrm{~m}, 0)\) and then returns along the same line to the point \((-20 \mathrm{~m}, 0)\). The distance and displacement of the particle during the trip are
The starting point for the particle is origin as shown in figure.
The Distance traveled by the particle is:
\(
\begin{array}{l}
\mathrm{D}=20+20+20 \\
=60 \mathrm{~m}
\end{array}
\)
The displacement is the distance between the initial and the final points. Displacement \(\Rightarrow \mathrm{OB}=20 \mathrm{~m}\) in the negative direction
The distance is \(60 \mathrm{~m}\) and displacement is \(20 \mathrm{~m}\) in negative direction.
A car has to cover the distance \(60 \mathrm{~km}\). If half of the total time, it travels with speed \(80 \mathrm{kmh}^{-1}\) and in rest half time, its speed becomes \(40 \mathrm{kmh}^{-1}\), the average speed of car will be
\(
\text { (a) } v_{\mathrm{av}}=\frac{\text { Total distance }}{\text { Total time }}=\frac{80 t+40 t}{2 t}=60 \mathrm{kmh}^{-1}
\)
During the first \(18 \mathrm{~min}\) of a \(60 \mathrm{~min}\) trip, a car has an average speed of \(11 \mathrm{~m} \mathrm{~min}^{-1}\). What should be the average speed for remaining \(42 \mathrm{~min}\), so that car is having an average speed of \(21 \mathrm{~m} \mathrm{~min}^{-1}\) for the entire trip?
\(
\begin{array}{l}
\text { (a) } 21=\frac{11 \times 18+42 \times v}{60} \\
\therefore \quad v=25.3 \mathrm{~m} \mathrm{~min}^{-1} \\
\end{array}
\)
A man walks on a straight road from his home to a market \(2.5 \mathrm{~km}\) away with a speed of \(5 \mathrm{kmh}^{-1}\). Finding the market closed, he instantly turns and walks back home with a speed of \(7.5 \mathrm{kmh}^{-1}\). The average speed of the man over the interval of time 0 to \(40 \mathrm{~min}\) is equal to
(d) Man walks from his home to market with a speed of \(5 \mathrm{kmh}^{-1}\). Distance \(=2.5 \mathrm{~km}\) and time \(=\frac{2.5}{5}=\frac{1}{2} \mathrm{~h}=30 \mathrm{~min}\) and he returns back with speed of \(7.5 \mathrm{~km} / \mathrm{h}\) in rest time, i.e. \(10 \mathrm{~min}\).
\(
\text { Distance }=7.5 \times \frac{10}{60}=1.25 \mathrm{~km}
\)
\(
\begin{aligned}
\text { So, average speed } & =\frac{\text { total distance }}{\text { total time }} \\
& =\frac{(2.5+1.25) \mathrm{km}}{(40 / 60) \mathrm{h}}=\frac{45}{8} \mathrm{kmh}^{-1}
\end{aligned}
\)
A particle is constrained to move on a straight line path. It returns to the starting point after \(10 \mathrm{~s}\). The total distance covered by the particle during this time is \(30 \mathrm{~m}\). Which of the following statements about the motion of the particle is true?
(d) Displacement of the particle will be zero because it comes back to its starting point.
\(
\text { Average speed }=\frac{\text { Total distance }}{\text { Total time }}=\frac{30 \mathrm{~m}}{10 \mathrm{~s}}=3 \mathrm{~ms}^{-1}
\)
A \(150 \mathrm{~m}\) long train is moving with a uniform velocity of \(45 \mathrm{kmh}^{-1}\). The time taken by the train to cross a bridge of length \(850 \mathrm{~m}\) is
\(
\text { (c) } t=\frac{d}{v}=\frac{150+850}{45 \times \frac{5}{18}}=80 \mathrm{~s}
\)
An insect crawls a distance of \(4 \mathrm{~m}\) along north in \(10 \mathrm{~s}\) and then a distance of \(3 \mathrm{~m}\) along east in \(5 \mathrm{~s}\). The average velocity of the insect is
\(
\text { (c) } v_{\mathrm{av}}=\frac{\text { Total displacement }}{\text { Total time }}=\frac{\sqrt{(4)^2+(3)^2}}{10+5}=\frac{1}{3} \mathrm{~ms}^{-1}
\)
A particle traversed (3/4) th of the circle of radius \(R\) in time \(t\). The magnitude of the average velocity of the particle in this time interval is
\(
\text { (c) } v_{\text {av }}=\frac{\text { Displacement }}{\text { Time }}=\frac{\sqrt{2} R}{t}
\)
A boy is running over a circular track with uniform speed of \(10 \mathrm{~ms}^{-1}\). What is the average velocity for movement of boy along semicircle (in \(\mathrm{ms}^{-1}\) )?
\(
\text { (d) } v_{\mathrm{av}}=\frac{\text { Displacement }}{\text { Time }}=\frac{2 R}{(\pi R / v)}=\frac{2 v}{\pi}=\frac{20}{\pi} \mathrm{ms}^{-1}
\)
Acceleration of a particle changes when
(c) Acceleration is a vector quantity. So, it changes when either magnitude or direction of velocity changes or both changes.
If a particle moves with an acceleration, then which of the following can remain constant?
(d) If the particle is accelerating then the velocity can not be constant. But the speed can be constant if the acceleration produced by the force is only change the direction of motion. For example in uniform circular motion, acceleration is non-zero, velocity is not constant but speed is constant.
The average velocity of a body moving with uniform acceleration travelling a distance of \(3.06 \mathrm{~m}\) is \(0.34 \mathrm{~ms}^{-1}\). If the change in velocity of the body is \(0.18 \mathrm{~ms}^{-1}\), then during this time, its uniform acceleration is
\(
\begin{array}{l}
\text { (b) } \text { Time }=\frac{\text { Distance }}{\text { Average velocity }}=\frac{3.06}{0.34}=9 \mathrm{~s} \\
\text { Acceleration }=\frac{\text { Change in velocity }}{\text { Time }}=\frac{0.18}{9}=0.02 \mathrm{~m} / \mathrm{s}^2
\end{array}
\)
A car travelling with a velocity of \(80 \mathrm{~km} / \mathrm{h}\) slowed down to \(44 \mathrm{~km} / \mathrm{h}\) in \(15 \mathrm{~s}\). The retardation is
(a)
\(
\begin{aligned}
a & =\frac{\text { Change in velocity }}{\text { Time taken }}=\frac{v_f-v_i}{t} \\
& =\frac{\left(44 \times \frac{5}{18}\right)-\left(80 \times \frac{5}{18}\right)}{15}=-0.67 \mathrm{~m} / \mathrm{s}^2
\end{aligned}
\)
Negative sign represents the retardation.
An object is moving along the path \(O A B O\) with constant speed, then
(d) For path \(O A\) and \(B O\), the magnitude of velocity (speed) and direction is constant, hence acceleration is zero.
For path \(A B\), since this path is a curve, so the direction of the velocity changes every moment but the magnitude of velocity (speed) remains constant.
Since, the direction of velocity is changing, i.e. there must be some acceleration along the path \(A B\).
Velocity of a body moving along a straight line with uniform acceleration \((a)\) reduces by \(\frac{3}{4}\) of its initial velocity in time \(t_0\). The total time of motion of the body till its velocity becomes zero is
(a)
\(
\begin{array}{l}
u-\frac{3 u}{4}=u-a t_0 \\
a=\frac{3 u}{4 t_0} \text { or } \frac{u}{a}=\frac{4}{3} t_0
\end{array}
\)
Now, \(0=u-a t\) or \(t=\frac{u}{a}=\frac{4}{3} t_0\)
The displacement of a body in \(8 \mathrm{~s}\) starting from rest with an acceleration of \(20 \mathrm{~cms}^{-2}\) is
\(
\text { (c) } s=\frac{1}{2} a t^2=\frac{1}{2} \times(0.2)(64)=6.4 \mathrm{~m}=640 \mathrm{~cm}
\)
The motion of a particle is described by the equation \(v=a t\). The distance travelled by the particle in the first \(4 \mathrm{~s}\) is
\(
\text { (d) } s=\frac{1}{2} a t^2 \Rightarrow s=\frac{1}{2} \times a \times(4)^2 \Rightarrow s=8 a
\)
A particle starts with a velocity of \(2 \mathrm{~ms}^{-1}\) and moves in a straight line with a retardation of \(0.1 \mathrm{~ms}^{-2}\). The first time at which the particle is \(15 \mathrm{~m}\) from the starting point is
\(
\text { (a) } 15=2 t-\frac{1}{2} \times(0.1) t^2 \text { or } t=10 \mathrm{~s}
\)
A particle starts from rest, accelerates at \(2 \mathrm{~ms}^{-2}\) for \(10 \mathrm{~s}\) and then moves with constant speed of \(20 \mathrm{~ms}^{-1}\) for \(30 \mathrm{~s}\) and then decelerates at \(4 \mathrm{~ms}^{-2}\) till it stops after next \(5 \mathrm{~s}\). What is the distance travelled by it?
(a)
\(
\begin{aligned}
s & =s_1+s_2+s_3 \\
& =\frac{1}{2} \times 2 \times(10)^2+(20)(30)+\frac{1}{2} \times 4 \times(5)^2 \\
& =100+600+50=750 \mathrm{~m}
\end{aligned}
\)
A body is moving with uniform velocity of \(8 \mathrm{~ms}^{-1}\). When the body just crossed another body, the second one starts and moves with uniform acceleration of \(4 \mathrm{~ms}^{-2}\). The time after which two bodies meet, will be
(b) Displacements of both should be equal.
or \(\quad 8 t=\frac{1}{2} \times 4 \times t^2\) or \(t=4 \mathrm{~s}\)
Two bodies \(A\) and \(B\) start from rest from the same point with a uniform acceleration of \(2 \mathrm{~ms}^{-2}\). If \(B\) starts one second later, then the two bodies are separated at the end of the next second, by
\(
\begin{array}{l}
\text { (c) } \quad s_B=\frac{1}{2} \times 2 \times(1)^2=1 \mathrm{~m} \\
s_A=\frac{1}{2} \times 2 \times(2)^2=4 \mathrm{~m} \\
\therefore \quad s_A-s_B=3 \mathrm{~m}
\end{array}
\)
A train accelerating uniformly from rest attains a maximum speed of \(40 \mathrm{~ms}^{-1}\) in \(20 \mathrm{~s}\). It travels at this speed for \(20 \mathrm{~s}\) and is brought to rest by uniform retardation in further \(40 \mathrm{~s}\). What is the average velocity during this period?
(c) \(\quad 40=(20) a_1 \Rightarrow a_1=2 \mathrm{~ms}^{-2}\)
Further \(40=(40) a_2\)
\(
\therefore \quad a_2=1 \mathrm{~ms}^{-2}
\)
Therefore, acceleration is \(2 \mathrm{~ms}^{-2}\) and retardation is \(1 \mathrm{~ms}^{-2}\).
\(
\text { Now, } \begin{aligned}
s_1 & =\frac{1}{2} a_1 t_1^2=\frac{1}{2} \times 2 \times(20)^2=400 \mathrm{~m} \\
s_2 & =v_{\max } t_2=40 \times 20=800 \mathrm{~m} \\
s_3 & =\frac{v_{\max }^2}{2 a_2}=\frac{(40)^2}{2 \times 1}=800 \mathrm{~m}
\end{aligned}
\)
\(
\begin{array}{l}
\text { Now, average velocity }=\frac{\text { total displacement }}{\text { total time }} \\
\qquad=\frac{400+800+800}{20+20+40}=25 \mathrm{~ms}^{-1}
\end{array}
\)
A particle starts from rest and traverses a distance \(l\) with uniform acceleration, then moves uniformly over a further distance \(2 l\) and finally comes to rest after moving a further distance \(3 l\) under uniform retardation. Assuming entire motion to be rectilinear motion, the ratio of average speed over the journey to the maximum speed on its ways is
(c) Let \(v_m\) be the maximum speed,
\(
\begin{array}{l}
v_m=a_1 t_1=\sqrt{2 a_1 l} (\because u=0) \\
t_2=\frac{2 l}{v_m} \text { and } v_m=a_2 t_3=\sqrt{2 a_2(3 l)}
\end{array}
\)
Now, average speed, \(v_{\mathrm{av}}=\frac{l+2 l+3 l}{t_1+t_2+t_3}\)
\(
\begin{aligned}
v_{\text {av }} & =\frac{6 l}{\left(v_m / a_1\right)+\left(2 l / v_m\right)+\left(v_m / a_2\right)} \\
& =\frac{6 l}{\left(\frac{v_m}{v_m^2 / 2 l}\right)+\left(\frac{2 l}{v_m}\right)+\left(\frac{v_m}{v_m^2 / 6 l}\right)}=\frac{6 l}{\left(10 l / v_m\right)}=\frac{3 v_m}{5} \\
\Rightarrow \quad \frac{v_{\text {av }}}{v_m} & =\frac{3}{5}
\end{aligned}
\)
A body travelling with uniform acceleration crosses two points \(A\) and \(B\) with velocities \(20 \mathrm{~ms}^{-1}\) and \(30 \mathrm{~ms}^{-1}\), respectively. The speed of the body at mid-point of \(A\) and \(B\) is
(b) \((30)^2=(20)^2+2 a(2 s)\) or \(\quad 2 a s=250\)
Now, \(v^2=u^2+2 a s \Rightarrow v^2=(20)^2+250 \Rightarrow v^2=650\)
\(
\therefore \quad v=25.5 \mathrm{~ms}^{-1}
\)
If a body starts from rest and travels \(120 \mathrm{~cm}\) in the 6th second, then what is the acceleration?
\(
\begin{array}{l}
\text { (c) } s_n=u+\frac{a}{2}(2 n-1) \Rightarrow 1.2=0+\frac{a}{2}(2 \times 6-1) \\
\Rightarrow a=\frac{1.2 \times 2}{11}=0.218 \mathrm{~ms}^{-2}
\end{array}
\)
If a stone is thrown up with a velocity of \(9.8 \mathrm{~ms}^{-1}\), then how much time will it take to come back?
\(
\text { (b) } t=\frac{2 u}{g} \Rightarrow t=\frac{2 \times 9.8}{10}=1.96 \approx 2 \mathrm{~s}
\)
If a ball is thrown vertically upwards with speed \(u\), the distance covered during the last \(t\) second of its ascent is
(d) Let \(t\) second of upward journey \(=\) first \(t\) second of downward journey (with zero initial velocity).
\(
\therefore \text { Desired distance }=\frac{1}{2} g t^2
\)
A person throws balls into air after every second. The next ball is thrown when the velocity of the first ball is zero. How high do the ball rise above his hand?
(b) Time taken to reach maximum height is \(1 \mathrm{~s}\).
Height \(=\) free fall distance in \(1 \mathrm{~s}=\frac{1}{2} g t^2=5 \mathrm{~m}\)
A particle is thrown vertically upwards. Its velocity at half of the height is \(10 \mathrm{~ms}^{-1}\). Then, the maximum height attained by it is (Take, \(g=10 \mathrm{~ms}^{-2}\) )
\(
\text { (b) } h=\frac{(10)^2}{2 g}=5 \mathrm{~m}
\)
\(
\therefore \text { Total height }=2 h=10 \mathrm{~m}
\)
When a ball is thrown up vertically with velocity \(v_0\), it reaches a maximum height of \(h\). If one wishes to triple the maximum height, then the ball should be thrown with velocity,
\(
\begin{array}{l}
\text { (a) } H_{\max } \propto v^2 \\
\Rightarrow \quad v \propto \sqrt{H_{\max }}
\end{array}
\)
i.e. To triple the maximum height, ball should be thrown with velocity \(\sqrt{3} v_0\).
A stone thrown upward with a speed \(u\) from the top of the tower reaches the ground with a speed \(3 u\). The height of the tower is
\(
\begin{aligned}
\text { (b) } & v^2Â =u^2+2 g h \\
\Rightarrow & (3 u)^2Â =(-u)^2+2 g h \\
\Rightarrow & h =\frac{4 u^2}{g}
\end{aligned}
\)
A body thrown vertically up from the ground passes the height of \(10.2 \mathrm{~m}\) twice in an interval of \(10 \mathrm{~s}\). What was its initial velocity?
\(
\text { (a) } t_{A B C}=10 \mathrm{~s} \Rightarrow t_{A B}=5 \mathrm{~s}
\)
At \(B\), velocity becomes zero. Hence at \(A\), velocity should be \(50 \mathrm{~ms}^{-1}\)
\(
\begin{array}{rlrl}
& \text { Now, } & (50)^2 & =\left(u^2\right)-2 \times 10 \times 10.2 \\
& \therefore & u & =52 \mathrm{~ms}^{-1}
\end{array}
\)
A body is projected with a velocity \(u\). It passes through a certain point above the ground after \(t_1\) second. The time interval after which the body passes through the same point during the return journey is
\(
\text { (b) Velocity of particle of this instant will be } v=(u-g 4)
\)
Now, the desired time interval will be \(\frac{2 v}{g}\). or \(\quad \frac{2\left(u-g t_1\right)}{g}=2\left(\frac{u}{g}-t_1\right)\)
A body is thrown vertically upwards from the top \(A\) of tower. It reaches the ground in \(t_1\) second. If it is thrown vertically downwards from \(A\) with the same speed, it reaches the ground in \(t_2\) second. If it is allowed to fall freely from \(A\), then the time it takes to reach the ground is given by
(c) Taking downward direction as the positive direction.
\(
\begin{array}{l}
+h=-u t_1+\frac{1}{2} g t_1^2 \dots(i) \\
+h=u t_2+\frac{1}{2} g t_2^2 \dots(ii)
\end{array}
\)
Multiplying Eq. (i) by \(t_2\) and Eq. (ii) by \(t_1\) and adding, we get
\(
h\left(t_1+t_2\right)=\frac{1}{2} g t_2 t_2\left(t_1+t_2\right) \text { or } h=\frac{1}{2} g t_1 t_2
\)
For free fall from rest, \(h=\frac{1}{2} g t^2\)
\(
\therefore \quad t^2=t_1 t_2 \Rightarrow t=\sqrt{t_1 t_2}
\)
A man in a balloon rising vertically with an acceleration of \(4.9 \mathrm{~ms}^{-2}\) releases a ball \(2 \mathrm{~s}\) after the balloon is let go from the ground. The greatest height above the ground reached by the ball is (Take, \(g=9.8 \mathrm{~ms}^{-2}\) )
(a) After \(2 \mathrm{~s}\), velocity, \(v=4.9 \times 2=9.8\)
and
\(
h=\frac{1}{2} \times 4.9 \times(2)^2=98 \mathrm{~m}
\)
Greatest height, \(h_{\max }=h+\frac{v^2}{2 g}=14.7 \mathrm{~m}\)
A stone falls freely under gravity. The total distance covered by it in the last second of its journey equals the distance covered by it in first \(3 \mathrm{~s}\) of its motion. The time for which stone remains in air, is
(a) Here, \(u=0\)
\(
\begin{aligned}
& S_3=0+\frac{1}{2} g t^2=\frac{1}{2} \times 10 \times 9=45 \\
S_{t \mathrm{th}} & =u+(2 t-1) \mathrm{g} / 2 \\
\Rightarrow S_{t \mathrm{th}} & =0+5(2 t-1) \\
45 & =5(2 t-1) \\
\Rightarrow 2 t-1 & =9 \Rightarrow t=5 \mathrm{~s}
\end{aligned}
\)
A body falls from a height \(h=200 \mathrm{~m}\). The ratio of distance travelled in each \(2 \mathrm{~s}\), during \(t=0\) to \(t=6 \mathrm{~s}\) of the journey is
\(
\begin{array}{l}
\text { (c) } \quad h_1=\frac{1}{2} \times g \times(2)^2=2 g \\
h_2=\frac{1}{2} \times g \times(4)^2-2 g=6 g \\
h_3=\frac{1}{2} \times g \times(6)^2-8 g=10 g \\
\therefore \quad h_1: h_2: h_3=1: 3: 5 \\
\end{array}
\)
A ball is released from height \(h\) and another from \(2 h\). The ratio of time taken by the two balls to reach the ground is
\(
\text { (a) } t=\sqrt{\frac{2 h}{g}} \text { or } t \propto \sqrt{h} \Rightarrow \frac{t_1}{t_2}=\sqrt{\frac{h}{2 h}}=1: \sqrt{2}
\)
A particle is dropped under gravity from rest from a height \(h\left(g=9.8 \mathrm{~ms}^{-2}\right)\) and it travels a distance \(9 h / 25\) in the last second, the height \(h\) is
\(
\text { (b) Let } h \text { be the distance covered in } t \text { second, } h=\frac{1}{2} g t^2 \quad \text {…(i) }
\)
\(
\begin{array}{l}
\text { Distance covered in } t \text { th second }=\frac{1}{2} g(2 t-1) \\
\Rightarrow \quad \frac{9 h}{25}=\frac{g}{2}(2 t-1) \dots(ii)
\end{array}
\)
From Eqs. (i) and (ii), we get
\(
h=122.5 \mathrm{~m}
\)
A body dropped from the top of a tower covers a distance \(7 x\) in the last second of its journey, where \(x\) is the distance covered in first second. How much time does it take to reach the ground?
(b) In first second distance travelled, \(x=\frac{1}{2} \times g \times t^2=5 \mathrm{~m}\) and similarly, in last second distance travelled, \(7 x=35 \mathrm{~m}\) Now, \(s_t=\left(u+a t-\frac{1}{2} a\right)\)
\(
\Rightarrow \quad 35=0+10 \times t-\frac{1}{2} \times 10
\)
\(
\therefore \quad t=4 \mathrm{~s}
\)
The displacement (in metre) of a particle moving along \(X\)-axis is given by \(x=18 t+5 t^2\). The average acceleration during the interval \(t_1=2 \mathrm{~s}\) and \(t_2=4 \mathrm{~s}\) is
\(
\begin{array}{l}
\text { (b) } x=18 t+5 t^2 \\
\quad v=\frac{d x}{d t}=\frac{d}{d t}\left(18 t+5 t^2\right)=18+10 t \\
\therefore \quad v=10 t+18 \\
\text { At } t_1=2 \mathrm{~s}, v_1=10(2)+18=38 \mathrm{~m} / \mathrm{s} \\
\text { At } t_2=4 \mathrm{~s}, v_2=10(4)+18=58 \mathrm{~m} / \mathrm{s} \\
\therefore \quad a=\frac{v_2-v_1}{t}=\frac{20}{2}=10 \mathrm{~m} / \mathrm{s}^2
\end{array}
\)
The displacement of a particle moving in a straight line is described by the relation \(s=6+12 t-2 t^2\). Here, \(s\) is in metre and \(t\) is in second. The distance covered by particle in first 5 \(s\) is
(d) \(v=\frac{d s}{d t}=12-4 t\)
Comparing with \(v=u+a t, u=12 \mathrm{~ms}^{-1}\) and \(a=-4 \mathrm{~ms}^{-2}\)
Velocity will become zero at time \(t_0 \Rightarrow 0=12-4 t_0\) or \(t_0=3 \mathrm{~s}\).
Since, the given time \(t=5 \mathrm{~s}\) is greater than \(t_0=3 \mathrm{~s}\)
distance \(>\mid\) displacement \(\mid\)
\(
\begin{array}{l}
\text { Distance, } d=\left|s_0-t_0\right|+\left|s_{t-t_0}\right|=\frac{u^2}{2|a|}+\frac{1}{2}|a|\left(t-t_0\right)^2 \\
=\frac{(12)^2}{8}+\frac{1}{2} \times 4 \times(2)^2=26 \mathrm{~m} \\
\end{array}
\)
The displacement of a particle moving in a straight line depends on time as \(x=\alpha t^3+\beta t^2+\gamma t+\delta\). The ratio of initial acceleration to its initial velocity depends on
\(
\text { (b) } v=\frac{d x}{d t}=\frac{d}{d t}\left(\alpha t^3+\beta t^2+\gamma t+\delta\right)
\)
\(
v=3 \alpha t^2+2 \beta t+\gamma ; v_{t=0}=v_i=\gamma
\)
\(
a=6 \alpha t+2 \beta: a_{t=0}=a_i=2 \beta
\)
\(
\therefore \quad \frac{v_i}{a_i}=\frac{\gamma}{2 \beta}
\)
The \(x\) and \(y\)-components of a position vector \(\mathbf{P}\) have numerical values 5 and 6, respectively. Direction and magnitude of vector \(\mathbf{P}\) are
(a) Vector \(\mathbf{P}\) is shown in the figure, then according to the given information,
\(
\begin{array}{cc}
& P_x=5, P_y=6 \\
\therefore & |\mathbf{P}|=\sqrt{P_x^2+P_y^2}=\sqrt{25+36} \\
\Rightarrow & |\mathbf{P}|=\sqrt{61} \\
\text { and } & \tan \theta=\frac{P_y}{P_x}=\frac{6}{5} \Rightarrow \theta=\tan ^{-1}\left(\frac{6}{5}\right)
\end{array}
\)
Thus, \(\mathbf{P}\) have magnitude of \(\sqrt{61}\) and lies in \(X Y\)-plane at an angle \(\tan ^{-1}\left(\frac{6}{5}\right)\) to the \(X\)-axis.
An object moves from positions \((6,8)\) to \((12,10)\) in the \(X Y\)-plane. Magnitude and direction of displacement is
(a) Positions of the object are
\(
\begin{aligned}
\mathbf{r}_1 & =6 \hat{\mathbf{i}}+8 \hat{\mathbf{j}} \text { and } \mathbf{r}_2=12 \hat{\mathbf{i}}+10 \hat{\mathbf{j}} \\
\therefore \Delta \mathbf{r} & =\mathbf{r}_2-\mathbf{r}_1=6 \hat{\mathbf{i}}+2 \hat{\mathbf{j}} \Rightarrow|\Delta \mathbf{r}|=\sqrt{40} \\
\theta & =\tan ^{-1}\left(\frac{\Delta y}{\Delta x}\right)=\tan ^{-1}\left(\frac{1}{3}\right)=1843^{\circ}
\end{aligned}
\)
A particle moves in \(X Y\)-plane from positions \((2 \mathrm{~m}, 4 \mathrm{~m})\) to \((6 \mathrm{~m}, 8 \mathrm{~m})\) is \(2 \mathrm{~s}\). Magnitude and direction of average velocity is
(b) Displacement, \(\Delta \mathbf{r}=\mathbf{r}_2-\mathbf{r}_1=4 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}\)
\(
\therefore \quad \mathbf{v}_{\mathrm{av}}=\frac{\Delta \mathbf{r}}{\Delta t}=\frac{4 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}}{2}=2(\hat{\mathbf{i}}+\hat{\mathbf{j}}) \mathrm{ms}^{-1}
\)
\(\Rightarrow\) Magnitude of velocity,
\(
\left|\mathbf{v}_{\text {av }}\right|=2 \sqrt{1^2+1^2}=2 \sqrt{2} \mathrm{~ms}^{-1}
\)
Direction, \(\theta=\tan ^{-1}\left(\frac{\Delta v_y}{\Delta v_x}\right)=\tan ^{-1}\left(\frac{2}{2}\right)=\tan ^{-1} 1=45^{\circ}\)
The displacement of an object along the three axes are given by, \(x=2 t^2, y=t^2-4 t\) and \(z=3 t-5\). The initial velocity of the particle is
\(
\begin{aligned}
(c) v_x & =4 t, v_y=2 t-4, v_z=3 \\
\text { At } t & =0, v_x=0, v_y=-4 \text { and } v_z=3 \\
\therefore \quad v & =\sqrt{v_y^2+v_z^2}=5 \text { units }
\end{aligned}
\)
A particle moves along the positive branch of the curve \(y=\frac{x^2}{2}\), where \(x=\frac{t^2}{2}, x\) and \(y\) are measured in metres and \(t\) in second. At \(t=2 \mathrm{~s}\), the velocity of the particle is
(c) As, \(\quad v_x=\frac{d x}{d t}=\frac{2 t}{2}=t\)
At \(t=2 \mathrm{~s}, \quad v_x=2 \mathrm{~ms}^{-1}\)
Further, \(\quad y=\frac{x^2}{2}=\frac{\left(t^2 / 2\right)^2}{2}=\frac{t^4}{8} \Rightarrow v_y=\frac{d y}{d t}=\frac{t^3}{2}\)
At \(t=2 \mathrm{~s}, v_y=4 \mathrm{~ms}^{-1}\)
So, velocity of particle is \((2 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}) \mathrm{ms}^{-1}\).
The position vector of a particle is
\(
\mathbf{r}=a \sin \omega t \hat{\mathbf{i}}+a \cos \omega t \hat{\mathbf{j}}
\)
The velocity of the particle is
\(
\begin{array}{l}
\text { (b) Given, } \mathbf{r}=(a \sin \omega t) \hat{\mathbf{i}}+(a \cos \omega t) \hat{\mathbf{j}} \\
\therefore \quad \mathbf{v}=\frac{d \mathbf{r}}{d t}=(-a \omega \sin \omega t) \hat{\mathbf{j}}+(a \omega \cos \omega t) \hat{\mathbf{i}} \\
\mathbf{r} \cdot \mathbf{v}=0 \Rightarrow \mathbf{r} \perp \mathbf{v} \\
\end{array}
\)
The position vector of an object at any time \(t\) is given by \(3 t^2 \hat{\mathbf{i}}+6 \hat{\mathbf{j}}+\hat{\mathbf{k}}\). Its velocity (in \(\mathrm{m} / \mathrm{s}\) ) along \(Y\)-axis has the magnitude
(c) Position vector, \(\mathbf{r}=3 t^2 \hat{\mathbf{i}}+6 \hat{\mathbf{j}}+\hat{\mathbf{k}}\)
Velocity vector, \(\mathbf{v}=\frac{d \mathbf{r}}{d t}=6 \hat{\mathbf{i}}+6 \hat{\mathbf{j}}+0=6 \hat{\mathbf{i}}+6 \hat{\mathbf{j}}\)
\(
\therefore \text { Magnitude of the velocity of the object along } Y \text {-axis }=6 \mathrm{~m} / \mathrm{s}
\)
The coordinates of a moving particle at any time \(t\) are given by, \(x=2 t^3\) and \(y=3 t^3\). Acceleration of the particle is given by
(b) Given, \(x=2 t^3\)
\(
\therefore \quad v_x=\frac{d x}{d t}=6 t^2 \Rightarrow a_x=\frac{d v_x}{d t}=12 t
\)
Also, \(y=3 t^3 \Rightarrow v_y=\frac{d y}{d t}=9 t^2 \Rightarrow a_y=\frac{d v_y}{d t}=18 t\)
\(\therefore\) Acceleration, \(a=\sqrt{a_x^2+a_y^2}=t \sqrt{468}\)
The position of a particle moving in the \(X Y\)-plane at any time \(t\) is given by \(x=\left(3 t^2-6 t\right) \mathrm{m}, y=\left(t^2-2 t\right) \mathrm{m}\). Select the correct statement about the moving particle from the following.
\(
\begin{aligned}
\text { (c) } v_x & =\frac{d x}{d t}=6 t-6, a_x=\frac{d v_x}{d t}=6 \mathrm{~ms}^{-2} \\
v_y & =2 t-2, \quad a_y=\frac{d v_y}{d t}=2 \mathrm{~ms}^{-2}
\end{aligned}
\)
At \(t=1 \mathrm{~s}, v_x\) and \(v_y\) both are zero. Hence, net velocity is zero.
A particle’s velocity changes from \((2 \hat{\mathbf{i}}+3 \hat{\mathbf{j}}) \mathrm{ms}^{-1}\) to \((3 \hat{\mathbf{i}}-2 \hat{\mathbf{j}}) \mathrm{ms}^{-1}\) in \(2 \mathrm{~s}\). Its average acceleration \(\left(\right.\) in \(\mathrm{ms}^{-2}\) ) is
\(
\text { (d) } \mathbf{a}_{\mathrm{av}}=\frac{\Delta \mathbf{v}}{\Delta t}=\frac{3 \hat{\mathbf{i}}-2 \hat{\mathbf{j}}-2 \hat{\mathbf{i}}-3 \hat{\mathbf{j}}}{2}=\frac{\hat{\mathbf{i}}-5 \hat{\mathbf{j}}}{2}
\)
A particle has an initial velocity of \(4 \hat{\mathbf{i}}+3 \hat{\mathbf{j}}\) and an acceleration of \(0.4 \hat{\mathbf{i}}+0.3 \hat{\mathbf{j}}\). Its speed after \(10 \mathrm{~s}\) is
\(
\begin{array}{l}
(a) \mathbf{v}=\mathbf{u}+\mathbf{a} t=(4 \hat{\mathbf{i}}+3 \hat{\mathbf{j}})+(0.4 \hat{\mathbf{i}}+0.3 \hat{\mathbf{j}})(10)=(8 \hat{\mathbf{i}}+6 \hat{\mathbf{j}}) \\
\therefore \quad v=\sqrt{(8)^2+(6)^2}=10 \text { units }
\end{array}
\)
A body lying initially at point \((3,7)\) starts moving with a constant acceleration of \(4 \hat{i}\). Its position after \(3 \mathrm{~s}\) is given by the coordinates
(c) Position vector of the body, \(\mathbf{r}=3 \hat{\mathbf{i}}+7 \hat{\mathbf{j}}\)
\(\because\) Acceleration of the body,
\(
\mathbf{a}=4 \hat{\mathbf{i}} \text { and } t=3 \mathrm{~s}
\)
Using \(\mathbf{s}=\mathbf{u}_0 t+\frac{1}{2} \mathbf{a} t^2=0 \times 3+\frac{4 \hat{\mathbf{i}}}{2} \times 3 \times 3 \Rightarrow \mathbf{s}=18 \hat{\mathbf{i}}\)
\(\therefore\) New position vector of the body,
\(
\mathbf{r}_1=3 \hat{\mathbf{i}}+7 \hat{\mathbf{j}}+18 \hat{\mathbf{i}}=21 \hat{\mathbf{i}}+7 \hat{\mathbf{j}}
\)
Coordinates becomes \((21,7)\)
The initial position of an object at rest is given by \(3 \hat{\mathbf{i}}-8 \hat{\mathbf{j}}\). It moves with constant acceleration and reaches to the position \(2 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}\) after \(4 \mathrm{~s}\). What is its acceleration?
(a) Initial position vector, \(\mathbf{r}_1=3 \hat{\mathbf{i}}-8 \hat{\mathbf{j}}\)
Final position vector, \(\mathbf{r}_2=2 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}\)
Change in position,
\(
\Delta \mathbf{r}=\mathbf{r}_2-\mathbf{r}_1=2 \hat{\mathbf{i}}+4 \hat{\mathbf{j}}-3 \hat{\mathbf{i}}+8 \hat{\mathbf{j}}=-\hat{\mathbf{i}}+12 \hat{\mathbf{j}}
\)
\(
\text { Using } \quad \mathbf{s}=\mathbf{u}_0 t+\frac{1}{2} \mathbf{a} t^2
\)
\(
\Rightarrow \quad-\hat{\mathbf{i}}+12 \hat{\mathbf{j}}=0+\frac{1}{2} \mathbf{a}(4)^2 \Rightarrow \mathbf{a}=\frac{-\hat{\mathbf{i}}+12 \hat{\mathbf{j}}}{8}=\frac{-\hat{\mathbf{i}}}{8}+\frac{3}{2} \hat{\mathbf{j}}
\)
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