Motion in a Straight Line

JEE Physics · 66 questions · Page 6 of 7 · Click an option or "Show Solution" to reveal answer

Q51
The position vector of a particle changes with time according to the relation r(t)=15t2i^+(420t2)j^\overrightarrow r (t) = 15{t^2}\widehat i + (4 - 20{t^2})\widehat j What is the magnitude of the acceleration at t = 1 ?
A 50
B 25
C 40
D 100
Correct Answer
Option A
Solution
r=(15t2)i^+(420t2)j^\overrightarrow r = \left( {15{t^2}} \right)\widehat i + \left( {4 - 20{t^2}} \right)\widehat j
v=drdt=(30t)i^(40t)j^\overrightarrow v = {{d\overrightarrow r } \over {dt}} = \left( {30t} \right)\widehat i - \left( {40t} \right)\widehat j
a=dvdt=(30)i^(40)j^\overrightarrow a = {{d\overrightarrow v } \over {dt}} = \left( {30} \right)\widehat i - \left( {40} \right)\widehat j
a=50\left| {\overrightarrow a } \right| = 50
Q52
An automobile travelling with speed of 60 km/h, can brake to stop within a distance of 20 m. If the car is going twice as fast, i.e 120 km/h, the stopping distance will be
A 60 m
B 40 m
C 20 m
D 80 m
Correct Answer
Option D
Solution

Assume

aa

be the retardation for both the vehicle then In case of automobile,

u122as1=0u_1^2 - 2a{s_1} = 0
u12=2as1\Rightarrow u_1^2 = 2a{s_1}

And in case for car,

u22=2as2u_2^2 = 2a{s_2}

\therefore

(u2u1)2=s2s1{\left( {{{{u_2}} \over {{u_1}}}} \right)^2} = {{{s_2}} \over {{s_1}}}
(12060)2=s220\Rightarrow {\left( {{{120} \over {60}}} \right)^2} = {{{s_2}} \over {20}}

\Rightarrow s2 = 80 m

Q53
The relation between time t and distance x is t = ax2 + bx where a and b are constants. The acceleration is
A 2bv3
B -2abv2
C 2av2
D -2av3
Correct Answer
Option D
Solution

The relationship between time t t and distance x x is defined as t=ax2+bx t = ax^2 + bx , where a a and b b are constants.

To find the acceleration, follow these steps: First, differentiate the equation with respect to time t t : ddt(t)=addt(x2)+bdxdt \dfrac{d}{dt}(t) = a \dfrac{d}{dt}(x^2) + b \dfrac{dx}{dt} This simplifies to: 1=a2xdxdt+bdxdt 1 = a \cdot 2x \dfrac{dx}{dt} + b \dfrac{dx}{dt} Given dxdt=v \dfrac{dx}{dt} = v (where v v is the velocity), we can write: 1=2axv+bv=v(2ax+b) 1 = 2axv + bv = v(2ax + b) This simplifies to: 2ax+b=1v 2ax + b = \dfrac{1}{v} Next, differentiate the expression 2ax+b=1v 2ax + b = \dfrac{1}{v} again with respect to t t : 2adxdt+0=1v2dvdt 2a \dfrac{dx}{dt} + 0 = -\dfrac{1}{v^2} \dfrac{dv}{dt} Using dxdt=v \dfrac{dx}{dt} = v , we get: 2av=1v2dvdt 2av = -\dfrac{1}{v^2} \dfrac{dv}{dt} Solving for dvdt \dfrac{dv}{dt} : dvdt=2av3 \dfrac{dv}{dt} = -2a v^3 Since acceleration f=dvdt f = \dfrac{dv}{dt} , we have: f=2av3 f = -2av^3

Q54
Two cars are travelling towards each other at speed of 20 m s120 \mathrm{~m} \mathrm{~s}^{-1} each. When the cars are 300 m300 \mathrm{~m} apart, both the drivers apply brakes and the cars retard at the rate of 2 m s22 \mathrm{~m} \mathrm{~s}^{-2}. The distance between them when they come to rest is :
A 25 m
B 100 m
C 50 m
D 200 m
Correct Answer
Option B
Solution

Let's analyze the given information before determining the distance between the two cars when they come to rest.

Each car is traveling towards the other at a speed of

20m s120 \, \text{m s}^{-1}

and they both start braking when they are

300m300 \, \text{m}

apart. The deceleration (negative acceleration) of each car is given as

2m s2.2 \, \text{m s}^{-2}.

To find the distance each car travels before coming to rest, we can use the kinematic equation that relates initial velocity (

viv_i

), final velocity (

vfv_f

), acceleration (

aa

), and distance (

dd

), which is:

vf2=vi2+2adv_f^2 = v_i^2 + 2ad

Since the final velocity

vf=0v_f = 0

(they come to rest), we can rearrange the equation to solve for

dd

(the distance each car travels before stopping):

0=vi2+2add=vi22a0 = v_i^2 + 2ad \Rightarrow d = -\frac{v_i^2}{2a}

Plugging in the values for each car (noting that acceleration

aa

is negative because it is deceleration, so

a=2m s2a = -2 \, \text{m s}^{-2}

):

d=(20)22(2)=4004=100md = -\frac{(20)^2}{2(-2)} = -\frac{400}{-4} = 100 \, \text{m}

Each car travels

100m100 \, \text{m}

before coming to rest. Since they both start

300m300 \, \text{m}

apart and each travels

100m100 \, \text{m}

towards the other, the total distance covered by both cars before stopping is

2×100m=200m2 \times 100 \, \text{m} = 200 \, \text{m}

.

To find the distance between them when they come to rest, we subtract the total distance covered by both cars from the original distance between them:

300m200m=100m300 \, \text{m} - 200 \, \text{m} = 100 \, \text{m}

So, the distance between the cars when they come to rest is

100m100 \, \text{m}

. Therefore, the correct option is: Option B 100 m

Q55
The co-ordinates of a moving particle at any time 't' are given by x = α\alpha t3 and y = βt3. The speed to the particle at time 't' is given by
A 3tα2+β23t\sqrt {{\alpha ^2} + {\beta ^2}}
B 3t2α2+β23{t^2}\sqrt {{\alpha ^2} + {\beta ^2}}
C t2α2+β2{t^2}\sqrt {{\alpha ^2} + {\beta ^2}}
D α2+β2\sqrt {{\alpha ^2} + {\beta ^2}}
Correct Answer
Option B
Solution

Given that

x=αt3x = \alpha {t^3}\,\,\,\,

and

y=βt3\,\,\,\,y = \beta {t^3}

\therefore

vx=dxdt=3αt2{v_x} = {{dx} \over {dt}} = 3\alpha {t^2}\,\,\,\,

and

vy=dydt=3βt2\,\,\,\,\,{v_y} = {{dy} \over {dt}} = 3\beta {t^2}

\therefore

v=vx2+vy2v = \sqrt {v_x^2 + v_y^2}
=9α2t4+9β2t4= \sqrt {9{\alpha ^2}{t^4} + 9{\beta ^2}{t^4}}
=3t2α2+β2= 3{t^2}\sqrt {{\alpha ^2} + {\beta ^2}}
Q56
Water drops are falling from a nozzle of a shower onto the floor, from a height of 9.8 m. The drops fall at a regular interval of time. When the first drop strikes the floor, at that instant, the third drop begins to fall. Locate the position of second drop from the floor when the first drop strikes the floor.
A 4.18 m
B 2.94 m
C 2.45 m
D 7.35 m
Correct Answer
Option D
Solution

H =

12{1 \over 2}

gt2

9.8×29.8{{9.8 \times 2} \over {9.8}}

= t2 t =

2\sqrt 2

sec

Δ\Delta

t : time interval between drops h =

12{1 \over 2}

g(

2\sqrt 2

- 2

Δ\Delta

t)2

Δ\Delta

t =

12{1 \over {\sqrt 2 }}

h =

12{1 \over 2}

g

(212)2=12×9.8×12=9.84=2.45{\left( {\sqrt 2 - {1 \over {\sqrt 2 }}} \right)^2} = {1 \over 2} \times 9.8 \times {1 \over 2} = {{9.8} \over 4} = 2.45

m H - h = 9.8 - 2.45 = 7.35 m

Q57
The distance travelled by an object in time tt is given by s=(2.5)t2s=(2.5) t^{2}. The instantaneous speed of the object at t=5 s\mathrm{t}=5 \mathrm{~s} will be:
A 5 ms15 \mathrm{~ms}^{-1}
B 12.5 ms112.5 \mathrm{~ms}^{-1}
C 62.5 ms162.5 \mathrm{~ms}^{-1}
D 25 ms125 \mathrm{~ms}^{-1}
Correct Answer
Option D
Solution

The distance traveled by an object in time

tt

is given by the equation

s=(2.5)t2s = (2.5)t^2

.

To find the instantaneous speed at a specific time, we need to find the first derivative of the distance function with respect to time, which gives us the velocity function:

v(t)=dsdtv(t) = \frac{ds}{dt}

Differentiating the given equation with respect to

tt

:

v(t)=ddt(2.5)t2=2(2.5)t=5tv(t) = \frac{d}{dt} (2.5)t^2 = 2(2.5)t = 5t

Now, we can find the instantaneous speed at

t=5 st = 5 \mathrm{~s}

by plugging the value into the velocity function:

v(5)=5(5)=25 m/sv(5) = 5(5) = 25 \mathrm{~m/s}

The instantaneous speed of the object at

t=5 st = 5 \mathrm{~s}

is

25 m/s25 \mathrm{~m/s}

.

Q58
Speeds of two identical cars are uu and 44uu at the specific instant. The ratio of the respective distances in which the two cars are stopped from that instant is :
A 1:11:1
B 1:41:4
C 1:81:8
D 1:161:16
Correct Answer
Option D
Solution

Given the initial speeds of two identical cars as uu and 4u4u, and considering that both cars eventually stop (final speed v=0v = 0), we note that both cars decelerate with the same acceleration a-a.

Using the kinematic equation: v2=u22as v^2 = u^2 - 2as Since v=0v = 0, 0=u22as 0 = u^2 - 2as Hence, u2=2as u^2 = 2as For the first car with speed uu, u2=2as1...(i) u^2 = 2a s_1 \quad \text{...(i)} For the second car with speed 4u4u, (4u)2=2as2...(ii) (4u)^2 = 2a s_2 \quad \text{...(ii)} Dividing equation (i) by equation (ii), u2(4u)2=2as12as2 \dfrac{u^2}{(4u)^2} = \dfrac{2a s_1}{2a s_2} u216u2=s1s2 \dfrac{u^2}{16u^2} = \dfrac{s_1}{s_2} 116=s1s2 \dfrac{1}{16} = \dfrac{s_1}{s_2} Thus, the ratio of the stopping distances of the two cars is 116\dfrac{1}{16}.

Q59
The position of a particle related to time is given by x=(5t24t+5)mx=\left(5 t^{2}-4 t+5\right) \mathrm{m}. The magnitude of velocity of the particle at t=2st=2 s will be :
A 14 ms114 \mathrm{~ms}^{-1}
B 16 ms116 \mathrm{~ms}^{-1}
C 10 ms110 \mathrm{~ms}^{-1}
D 06 ms106 \mathrm{~ms}^{-1}
Correct Answer
Option B
Solution

The position of a particle as a function of time is given by x=(5t24t+5)mx=\left(5 t^{2}-4 t+5\right) \mathrm{m}.

To find the magnitude of the velocity of the particle at t=2st=2\,\mathrm{s}, we first need to find the velocity of the particle as a function of time.

The velocity vv is the time derivative of the position xx:

v=dxdtv = \frac{dx}{dt}

Taking the derivative of xx with respect to tt, we get:

v=dxdt=10t4m/sv = \frac{dx}{dt} = 10t - 4\,\mathrm{m/s}

Now we can find the velocity of the particle at t=2st=2\,\mathrm{s} by plugging in t=2t=2:

v(2s)=10(2)4m/s=16m/sv(2\,\mathrm{s}) = 10(2) - 4\,\mathrm{m/s} = 16\,\mathrm{m/s}

Therefore, the magnitude of the velocity of the particle at t=2st=2\,\mathrm{s} is:

v(2s)=16m/s\boxed{|v(2\,\mathrm{s})| = 16\,\mathrm{m/s}}
Q60
A particle moves from the point (2.0i^+4.0j^)\left( {2.0\widehat i + 4.0\widehat j} \right) m, at t = 0, with an initial velocity (5.0i^+4.0j^)\left( {5.0\widehat i + 4.0\widehat j} \right) ms-1. It is acted upon by a constant force which produces a constant acceleration (4.0i^+4.0j^)\left( {4.0\widehat i + 4.0\widehat j} \right) ms-2. What is the distance of the particle from the origin at time 2 s?
A 15 m
B 20220\sqrt 2 m
C 10210\sqrt 2 m
D 5 m
Correct Answer
Option B
Solution
S=(5i^+4)2+12(4i^+4j^)4\overrightarrow S = \left( {5\widehat i + 4} \right)2 + {1 \over 2}\left( {4\widehat i + 4\widehat j} \right)4
=10i^+8j^+8i^+8j^= 10\widehat i + 8\widehat j + 8\widehat i + 8\widehat j
rfri=18i^+16j^\overrightarrow {{r_f}} - \overrightarrow {{r_i}} = 18\widehat i + 16\widehat j
rf=20i^+20j^\overrightarrow {{r_f}} = 20\widehat i + 20\widehat j
rf=202\left| {\overrightarrow {{r_f}} } \right| = 20\sqrt 2
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