Motion in a Plane

NEET Physics · 49 questions · Page 1 of 5 · Click an option or "Show Solution" to reveal answer

Q1
A bob is whirled in a horizontal circle by means of a string at an initial speed of 10 rpm10 \mathrm{~rpm}. If the tension in the string is quadrupled while keeping the radius constant, the new speed is:
A 20 rpm
B 40 rpm
C 5 rpm
D 10 rpm
Correct Answer
Option A
Solution

To solve this problem, we need to understand the relationship between the tension in the string and the speed of the bob whirling in a horizontal circle.

The centripetal force acting on the bob is provided by the tension in the string, and it can be given by the formula:

F=mv2rF = \frac{m v^2}{r}

where: F is the centripetal force (or tension in the string) m is the mass of the bob v is the tangential speed of the bob r is the radius of the circle According to the problem, the initial speed of the bob is

10 rpm10 \mathrm{~rpm}

, and the radius is kept constant. Let’s denote the initial tension in the string as

T1T_1

and the new tension as

T2T_2

. Given that the tension in the string is quadrupled, we have:

T2=4T1T_2 = 4 T_1

Also, the centripetal force can be written in terms of tension:

T1=mv12rT_1 = \frac{m v_1^2}{r}
T2=mv22rT_2 = \frac{m v_2^2}{r}

By substituting

T2=4T1T_2 = 4 T_1

into the second equation, we get:

4T1=mv22r4 T_1 = \frac{m v_2^2}{r}

We know from the first equation that:

T1=mv12rT_1 = \frac{m v_1^2}{r}

Substituting this into our equation for

T2T_2

:

4(mv12r)=mv22r4 \left(\frac{m v_1^2}{r}\right) = \frac{m v_2^2}{r}

The masses and radii cancel out, leaving us with:

4v12=v224 v_1^2 = v_2^2

Taking the square root of both sides:

v2=2v1v_2 = 2 v_1

The initial speed

v1v_1

is given as

10 rpm10 \mathrm{~rpm}

. Therefore, the new speed

v2v_2

is:

v2=2×10 rpm=20 rpmv_2 = 2 \times 10 \mathrm{~rpm} = 20 \mathrm{~rpm}

Hence, the new speed of the bob is 20 rpm . The correct answer is Option A.

Q2
Let ω1,ω2\omega_1, \omega_2 and ω3\omega_3 be the angular speed of the second hand, minute hand and hour hand of a smoothly running analog clock, respectively. If x1,x2x_1, x_2 and x3x_3 are their respective angular distances in 1 minute then the factor which remains constant (k)(k) is
A ω1x1=ω2x2=ω3x3=k\dfrac{\omega_1}{x_1}=\dfrac{\omega_2}{x_2}=\dfrac{\omega_3}{x_3}=k
B ω1x1=ω2x2=ω3x3=k\omega_1 x_1=\omega_2 x_2=\omega_3 x_3=k
C ω1x12=ω2x22=ω3x32=k\omega_1 x_1^2=\omega_2 x_2^2=\omega_3 x_3^2=k
D ω12x1=ω22x2=ω32x3=k\omega_1^2 x_1=\omega_2^2 x_2=\omega_3^2 x_3=k
Correct Answer
Option A
Solution
ω1=2π60;x1=2π60×60=2πω2=2π3600;x2=2π3600×60=2π60ω3=2π3600×12;x3=2π3600×12×60=2π720ω1x1=ω2x2=ω3x3=160=k\begin{aligned} & \omega_1=\frac{2 \pi}{60} ; \quad x_1=\frac{2 \pi}{60} \times 60=2 \pi \\\\ & \omega_2=\frac{2 \pi}{3600} ; \quad x_2=\frac{2 \pi}{3600} \times 60=\frac{2 \pi}{60} \\\\ & \omega_3=\frac{2 \pi}{3600 \times 12} ; \quad x_3=\frac{2 \pi}{3600 \times 12} \times 60=\frac{2 \pi}{720} \\\\ & \frac{\omega_1}{x_1}=\frac{\omega_2}{x_2}=\frac{\omega_3}{x_3}=\frac{1}{60}=k \end{aligned}
Q3
A ball is projected from point A with velocity 20 m s120 \mathrm{~m} \mathrm{~s}^{-1} at an angle 6060^{\circ} to the horizontal direction. At the highest point B\mathrm{B} of the path (as shown in figure), the velocity vms1\mathrm{v} \mathrm{m} \mathrm{s}^{-1} of the ball will be:
A 20
B 10310 \sqrt{3}
C Zero
D 10
Correct Answer
Option D
Solution

At the top most point of its trajectory particle will have only horizontal component of velocity

V at top =vcosθ=20×12=10 m/s\begin{aligned} & \mathrm{V} \text{ at top }=v \cos \theta \\ & =20 \times \frac{1}{2} \\ & =10 \mathrm{~m} / \mathrm{s} \end{aligned}
Q4
A particle is executing uniform circular motion with velocity v\vec{v} and acceleration a\vec{a}. Which of the following is true?
A v\vec{v} is a constant; a\vec{a} is not a constant
B v\vec{v} is not a constant; a\vec{a} is not a constant
C v\vec{v} is a constant; a\vec{a} is a constant
D v\vec{v} is not a constant; a\vec{a} is a constant
Correct Answer
Option B
Solution

Direction of velocity and centripetal acceleration changes continuously so

v\vec{v}

is not constant and

a\vec{a}

is not a constant.

Q5
A bullet is fired from a gun at the speed of 280 ms1280 \mathrm{~ms}^{-1} in the direction 3030^{\circ} above the horizontal. The maximum height attained by the bullet is (g=9.8 ms2,sin30=0.5)\left(g=9.8 \mathrm{~ms}^{-2}, \sin 30^{\circ}=0.5\right):-
A 2000 m
B 1000 m
C 3000 m
D 2800 m
Correct Answer
Option B
Solution
Hmax=u2sin2θ2g\mathrm{H}_{\max }=\frac{\mathrm{u}^{2} \sin ^{2} \theta}{2 g}
=(280)2(sin30)22(9.8)=\frac{(280)^{2}\left(\sin 30^{\circ}\right)^{2}}{2(9.8)}
=1000 m=1000 \mathrm{~m}
Q6
A horizontal bridge is built across a river. A student standing on the bridge throws a small ball vertically upwards with a velocity 4 m s14 \mathrm{~m} \mathrm{~s}^{-1}. The ball strikes the water surface after 4 s4 \mathrm{~s}. The height of bridge above water surface is (Take g=10 m s2g=10 \mathrm{~m} \mathrm{~s}^{-2} )
A 60 m
B 64 m
C 68 m
D 56 m
Correct Answer
Option B
Solution
S=ut+12at2S=u t+\frac{1}{2} a t^{2}
H=4×412×10×42-\mathrm{H}=4 \times 4-\frac{1}{2} \times 10 \times 4^{2}
H=1680-\mathrm{H}=16-80
H=64-\mathrm{H}=-64
H=64 m\mathrm{H}=64 \mathrm{~m}
Q7
A cricket ball is thrown by a player at a speed of 20 m/s in a direction 30^\circ above the horizontal. The maximum height attained by the ball during its motion is (g = 10 m/s 2 )
A 25 m
B 5 m
C 10 m
D 20 m
Correct Answer
Option B
Solution

Maximum height reached by the ball

H=v2sin2θ2gH = {{{v^2}{{\sin }^2}\theta } \over {2g}}
=(20)2sin2302g= {{{{(20)}^2}{{\sin }^2}30^\circ } \over {2g}}
H=5mH = 5\,m
Q8
A ball is projected with a velocity, 10 ms -1 , at an angle of 60^\circ with the vertical direction. Its speed at the highest point of its trajectory will be
A Zero
B 53\sqrt3 ms -1
C 5 ms -1
D 10 ms -1
Correct Answer
Option B
Solution

At highest point vertical component of velocity become zero. At highest point speed of object = 10cos30

^\circ

= 5

3\sqrt3

m/s

Q9
A particle moving in a circle of radius R with a uniform speed takes a time T to complete one revolution. If this particle were projected with the same speed at an angle 'θ\theta' to the horizontal, the maximum height attained by it equals 4R. The angle of projection, θ\theta, is then given by :
A θ=sin1(2gT2π2R)1/2\theta = {\sin ^{ - 1}}{\left( {{{2g{T^2}} \over {{\pi ^2}R}}} \right)^{1/2}}
B θ=cos1(gT2π2R)1/2\theta = {\cos ^{ - 1}}{\left( {{{g{T^2}} \over {{\pi ^2}R}}} \right)^{1/2}}
C θ=cos1(π2RgT2)1/2\theta = {\cos ^{ - 1}}{\left( {{{{\pi ^2}R} \over {g{T^2}}}} \right)^{1/2}}
D θ=sin1(π2RgT2)1/2\theta = {\sin ^{ - 1}}{\left( {{{{\pi ^2}R} \over {g{T^2}}}} \right)^{1/2}}
Correct Answer
Option A
Solution
T=2πRVT = {{2\pi R} \over V}
V=2πRTV = {{2\pi R} \over T}
H=u2sin2θ2gH = {{{u^2}{{\sin }^2}\theta } \over {2g}}
4R=4π2R2sin2θT22g4R = {{4{\pi ^2}{R^2}{{\sin }^2}\theta } \over {{T^2}2g}}
sin2θ=8RT2g4π2R2{\sin ^2}\theta = {{8R{T^2}g} \over {4{\pi ^2}{R^2}}}
sin2θ=2T2gπ2R{\sin ^2}\theta = \sqrt {{{2{T^2}g} \over {{\pi ^2}R}}}
θ=sin1(2T2gπ2R)1/2\theta = {\sin ^{ - 1}}{\left( {{{2{T^2}g} \over {{\pi ^2}R}}} \right)^{1/2}}
Q10
A car starts from rest and accelerates at 5m/s 2 . At t = 4 s, a ball is dropped out of a window by a person sitting in the car. What is the velocity and acceleration of the ball at t = 6 s? (Take g = 10 m/s 2 )
A 202\sqrt 2 m/s, 10 m/s 2
B 20 m/s, 5 m/s 2
C 20 m/s, 0
D 202\sqrt 2 m/s, 0
Correct Answer
Option A
Solution

u = 0 a = 5 t = 4 velocity of car at t = 4 sec is V = u + at V = 0 + 5 ×\times 4 V = 20 m/s For ball : At t = 4 s, A ball is dropped out of a window so velocity of ball at this instant is 20 ms–1 along horizontal.

After 2 seconds of motion : Horizontal velocity of ball , V x = 20 m/sec V y = u + ut = 10 ×\times 2 Vertical velocity of ball, V y = 20 m/sec So magnitude of velocity of ball V =

Vx2+Vy2\sqrt {V_x^2 + V_y^2}

= 20

2\sqrt 2

and Acceleration of ball at t = 6 s is g = 10 m/sec 2 As ball is under free fall.

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