Motion in a Plane

JEE Physics · 62 questions · Page 5 of 7 · Click an option or "Show Solution" to reveal answer

Q41
A child stands on the edge of the cliff 10 m10 \mathrm{~m} above the ground and throws a stone horizontally with an initial speed of 5 ms15 \mathrm{~ms}^{-1}. Neglecting the air resistance, the speed with which the stone hits the ground will be ms1\mathrm{ms}^{-1} (given, g=10 ms2g=10 \mathrm{~ms}^{-2} ).
A 20
B 25
C 30
D 15
Correct Answer
Option D
Solution
vy=2gh=200vnet=25+200=15 m/s\begin{aligned} & \mathrm{v}_{\mathrm{y}}=\sqrt{2 g h}=\sqrt{200} \\\\ & v_{n e t}=\sqrt{25+200}=15 \mathrm{~m} / \mathrm{s} \end{aligned}
Q42
Two objects are projected with same velocity 'u' however at different angles α\alpha and β\beta with the horizontal. If α+β=90\alpha+\beta=90^\circ, the ratio of horizontal range of the first object to the 2nd object will be :
A 1 : 1
B 2 : 1
C 1 : 2
D 4 : 1
Correct Answer
Option A
Solution
Range=u2sin2θg\text{Range}=\frac{u^2 \sin 2 \theta}{g}

Range for projection angle " α\alpha "

R1=u2sin2αg\mathrm{R}_1=\frac{\mathrm{u}^2 \sin 2 \alpha}{\mathrm{g}}

Range for projection angle " β\beta "

R2=u2sin2βgα+β=90( Given )β=90αR2=u2sin2(90α)gR2=u2sin(1802α)gR2=u2sin2αgR1R2=(u2sin2αg)(u2sin2αg)=11\begin{aligned} & \mathrm{R}_2=\frac{\mathrm{u}^2 \sin 2 \beta}{\mathrm{g}} \\\\ & \alpha+\beta=90^{\circ}(\text{ Given }) \\\\ & \Rightarrow \beta=90^{\circ}-\alpha \\\\ & \mathrm{R}_2=\frac{\mathrm{u}^2 \sin 2\left(90^{\circ}-\alpha\right)}{\mathrm{g}} \\\\ & \mathrm{R}_2=\frac{\mathrm{u}^2 \sin \left(180^{\circ}-2 \alpha\right)}{\mathrm{g}} \\\\ & \mathrm{R}_2=\frac{\mathrm{u}^2 \sin 2 \alpha}{\mathrm{g}} \\\\ & \Rightarrow \frac{\mathrm{R}_1}{\mathrm{R}_2}=\frac{\left(\frac{\mathrm{u}^2 \sin 2 \alpha}{\mathrm{g}}\right)}{\left(\frac{\mathrm{u}^2 \sin 2 \alpha}{\mathrm{g}}\right)}=\frac{1}{1} \end{aligned}
Q43
A projectile is projected at 3030^{\circ} from horizontal with initial velocity 40 ms140 \mathrm{~ms}^{-1}. The velocity of the projectile at t=2 s\mathrm{t}=2 \mathrm{~s} from the start will be : (Given g=10 m/s2g=10 \mathrm{~m} / \mathrm{s}^{2} )
A 203 ms120 \sqrt{3} \mathrm{~ms}^{-1}
B Zero
C 20 ms120 \mathrm{~ms}^{-1}
D 403 ms140 \sqrt{3} \mathrm{~ms}^{-1}
Correct Answer
Option A
Solution

To find the velocity of the projectile at t = 2 s, we need to find the horizontal and vertical components of the velocity at that time.

The initial horizontal component of the velocity is constant and is given by:

v0x=v0cosθ=40ms1cos(30)=40ms132=203ms1v_{0x} = v_0 \cos\theta = 40\,\mathrm{ms}^{-1} \cos(30^{\circ}) = 40\,\mathrm{ms}^{-1} \cdot \frac{\sqrt{3}}{2} = 20\sqrt{3}\,\mathrm{ms}^{-1}

The initial vertical component of the velocity is:

v0y=v0sinθ=40ms1sin(30)=40ms112=20ms1v_{0y} = v_0 \sin\theta = 40\,\mathrm{ms}^{-1} \sin(30^{\circ}) = 40\,\mathrm{ms}^{-1} \cdot \frac{1}{2} = 20\,\mathrm{ms}^{-1}

To find the vertical component of the velocity at t = 2 s, we use the equation:

vy=v0ygt=20ms1(10ms2)(2s)=20ms120ms1=0ms1v_y = v_{0y} - gt = 20\,\mathrm{ms}^{-1} - (10\,\mathrm{ms}^{-2})(2\,\mathrm{s}) = 20\,\mathrm{ms}^{-1} - 20\,\mathrm{ms}^{-1} = 0\,\mathrm{ms}^{-1}

At t = 2 s, the horizontal component of the velocity is still

203ms120\sqrt{3}\,\mathrm{ms}^{-1}

, and the vertical component is 0. The overall velocity at t = 2 s is:

v=203ms1i^+0ms1j^=203ms1\vec{v} = 20\sqrt{3}\,\mathrm{ms}^{-1} \hat{i} + 0\,\mathrm{ms}^{-1} \hat{j} = 20\sqrt{3}\,\mathrm{ms}^{-1}

So the correct answer is:

203ms120\sqrt{3}\,\mathrm{ms}^{-1}
Q44
Two projectiles are projected at 3030^{\circ} and 6060^{\circ} with the horizontal with the same speed. The ratio of the maximum height attained by the two projectiles respectively is:
A 1:31: \sqrt{3}
B 3:1\sqrt{3}: 1
C 1 : 3
D 2:32: \sqrt{3}
Correct Answer
Option C
Solution

Let the initial speed of both projectiles be v.

The maximum height attained by a projectile can be calculated using the formula:

H=v2sin2θ2gH = \frac{v^2 \sin^2 \theta}{2g}

where H is the maximum height, v is the initial speed, θ is the angle of projection, and g is the acceleration due to gravity.

For the projectile projected at 30°, the maximum height is:

H1=v2sin2302g=v2×142g=v28gH_1 = \frac{v^2 \sin^2 30^{\circ}}{2g} = \frac{v^2 \times \frac{1}{4}}{2g} = \frac{v^2}{8g}

For the projectile projected at 60°, the maximum height is:

H2=v2sin2602g=v2×342g=3v28gH_2 = \frac{v^2 \sin^2 60^{\circ}}{2g} = \frac{v^2 \times \frac{3}{4}}{2g} = \frac{3v^2}{8g}

Now, let's find the ratio of the maximum heights:

H1H2=v28g3v28g=v23v2\frac{H_1}{H_2} = \frac{\frac{v^2}{8g}}{\frac{3v^2}{8g}} = \frac{v^2}{3v^2}

The v² terms cancel out, and we get:

H1H2=13\frac{H_1}{H_2} = \frac{1}{3}

Therefore, the ratio of the maximum heights attained by the two projectiles is 1 : 3

Q45
The range of the projectile projected at an angle of 15^\circ with horizontal is 50 m. If the projectile is projected with same velocity at an angle of 45^\circ with horizontal, then its range will be
A 502\sqrt2 m
B 100 m
C 1002\sqrt2 m
D 50 m
Correct Answer
Option B
Solution

The range RR of a projectile launched with an initial speed vv and at an angle θ\theta to the horizontal is given by: R=v2gsin(2θ)R = \dfrac{v^2}{g} \sin(2\theta) where gg is the acceleration due to gravity.

From this equation, we can see that the range is dependent on the sine of twice the launch angle.

Given that the range at 1515^\circ is 5050 m, if we launch the projectile at 4545^\circ with the same velocity, we can compare the ranges by comparing sin(2×15)\sin(2 \times 15^\circ) and sin(2×45)\sin(2 \times 45^\circ): sin(30)=12\sin(30^\circ) = \dfrac{1}{2} sin(90)=1\sin(90^\circ) = 1 Therefore, the range at 4545^\circ will be twice the range at 1515^\circ, because sin(90)\sin(90^\circ) is twice as large as sin(30)\sin(30^\circ).

So, the range when the projectile is launched at 4545^\circ will be 2×502 \times 50 m = 100100 m.

So, 100100 m is the correct answer.

Q46
The trajectory of projectile, projected from the ground is given by y=xx220y=x-\dfrac{x^{2}}{20}. Where xx and yy are measured in meter. The maximum height attained by the projectile will be.
A 10 m
B 5 m
C 200 m
D 102\sqrt2 m
Correct Answer
Option B
Solution

The equation of the trajectory given is y=xx220y = x - \dfrac{x^2}{20}.

This is a parabola, and it represents the path of the projectile.

The maximum height of the projectile corresponds to the vertex of the parabola.

The x-coordinate of the vertex for a parabola given by y=ax2+bx+cy = ax^2 + bx + c is b/2a-b/2a.

In this case, a=1/20a = -1/20 and b=1b = 1, so the x-coordinate of the vertex is: xvertex=b2a=12×(1/20)=10 x_{\text{vertex}} = -\dfrac{b}{2a} = -\dfrac{1}{2 \times (-1/20)} = 10 Substituting this into the equation of the trajectory gives the y-coordinate of the vertex, which is the maximum height: ymax=1010220=105=5 y_{\text{max}} = 10 - \dfrac{10^2}{20} = 10 - 5 = 5 So, the maximum height attained by the projectile is 5 m.

Q47
Two projectiles A and B are thrown with initial velocities of 40 m/s40 \mathrm{~m} / \mathrm{s} and 60 m/s60 \mathrm{~m} / \mathrm{s} at angles 3030^{\circ} and 6060^{\circ} with the horizontal respectively. The ratio of their ranges respectively is (g=10 m/s2)\left(g=10 \mathrm{~m} / \mathrm{s}^{2}\right)
A 4:94: 9
B 2:32: \sqrt{3}
C 3:2\sqrt{3}: 2
D 1:11: 1
Correct Answer
Option A
Solution

The range of a projectile launched with an initial velocity vv at an angle θ\theta with respect to the horizontal is given by: R=v2sin(2θ)gR = \dfrac{v^2 \sin(2\theta)}{g}, where gg is the acceleration due to gravity.

Let's calculate the ranges of projectiles A and B: For projectile A, v=40m/sv = 40 \, \text{m/s} and θ=30\theta = 30^\circ, so: RA=(40)2sin(2×30)10=4×40=160mR_A = \dfrac{(40)^2 \sin(2 \times 30)}{10} = 4 \times 40 = 160 \, \text{m}.

For projectile B, v=60m/sv = 60 \, \text{m/s} and θ=60\theta = 60^\circ, so: RB=(60)2sin(2×60)10=6×60=360mR_B = \dfrac{(60)^2 \sin(2 \times 60)}{10} = 6 \times 60 = 360 \, \text{m}.

Therefore, the ratio of their ranges is RA:RB=160:360=4:9R_A : R_B = 160 : 360 = 4 : 9.

Q48
Given below are two statements : one is labelled as Assertion A and the other is labelled as Reason R Assertion A : When a body is projected at an angle 4545^{\circ}, it's range is maximum. Reason R : For maximum range, the value of sin2θ\sin 2 \theta should be equal to one. In the light of the above statements, choose the correct answer from the options given below:
A Both A\mathbf{A} and R\mathbf{R} are correct and R\mathbf{R} is the correct explanation of A\mathbf{A}
B A\mathbf{A} is true but R\mathbf{R} is false
C A\mathbf{A} is false but R\mathbf{R} is true
D Both A\mathbf{A} and R\mathbf{R} are correct but R\mathbf{R} is NOT the correct explanation of A\mathbf{A}
Correct Answer
Option A
Solution

Assertion A: When a body is projected at an angle of 4545^{\circ}, its range is maximum.

This is true, and it's a well-established fact in physics.

The maximum range of a projectile, assuming no air resistance and flat terrain, is achieved at an angle of 4545^{\circ}.

Reason R: For maximum range, the value of sin2θ\sin 2\theta should be equal to one.

This is also true.

The range of a projectile, again assuming no air resistance and flat terrain, can be calculated using the formula R=(v2/g)sin(2θ)R = (v^{2}/g) \cdot \sin(2\theta), where vv is the initial velocity of the projectile, gg is the acceleration due to gravity, and θ\theta is the launch angle.

For the range to be maximized, sin(2θ)\sin(2\theta) must be maximized, and the maximum value of sin(2θ)\sin(2\theta) is 1.

This occurs when 2θ=902\theta = 90 degrees, or θ=45\theta = 45 degrees, which corresponds to the assertion.

Q49
Position of an ant (S\mathrm{S} in metres) moving in Y\mathrm{Y}-Z\mathrm{Z} plane is given by S=2t2j^+5k^S=2 t^2 \hat{j}+5 \hat{k} (where tt is in second). The magnitude and direction of velocity of the ant at t=1 s\mathrm{t}=1 \mathrm{~s} will be :
A 16 m/s16 \mathrm{~m} / \mathrm{s} in yy-direction
B 4 m/s4 \mathrm{~m} / \mathrm{s} in xx-direction
C 9 m/s9 \mathrm{~m} / \mathrm{s} in z\mathrm{z}-direction
D 4 m/s4 \mathrm{~m} / \mathrm{s} in yy-direction
Correct Answer
Option D
Solution

The position of an ant, denoted as S \mathrm{S} in meters, moving in the Y \mathrm{Y} -Z \mathrm{Z} plane is given by S=2t2j^+5k^ S = 2t^2 \hat{j} + 5 \hat{k} , where t t is in seconds.

To determine the magnitude and direction of the ant's velocity at t=1 t = 1 second, we need to differentiate the position function with respect to time.

The velocity v \overrightarrow{\mathrm{v}} is given by:

v=dSdt=ddt(2t2j^+5k^)\overrightarrow{\mathrm{v}} = \frac{d\mathrm{S}}{dt} = \frac{d}{dt} (2t^2 \hat{j} + 5 \hat{k})

On differentiating, we get:

v=4tj^\overrightarrow{\mathrm{v}} = 4t \hat{j}

At t=1 t = 1 second:

v=41j^=4j^\overrightarrow{\mathrm{v}} = 4 \cdot 1 \hat{j} = 4 \hat{j}

Therefore, the magnitude of the velocity is 4 m/s 4 \mathrm{~m/s} and it is directed along the y y -axis.

Q50
The co-ordinates of a particle moving in xx-yy plane are given by : x=2+4t,y=3t+8t2x=2+4 \mathrm{t}, y=3 \mathrm{t}+8 \mathrm{t}^2. The motion of the particle is :
A uniform motion along a straight line.
B non-uniformly accelerated.
C uniformly accelerated having motion along a straight line.
D uniformly accelerated having motion along a parabolic path.
Correct Answer
Option D
Solution

To determine the nature of the motion of the particle given by its coordinates in the

xx

-

yy

plane, we analyze the given equations for

xx

and

yy

in terms of time

tt

:

x=2+4tx = 2 + 4t
y=3t+8t2y = 3t + 8t^2

Firstly, the equation for

xx

is of the form

x=x0+vtx = x_0 + vt

, where

x0=2x_0 = 2

is the initial position and

v=4v = 4

is the constant velocity along the

xx

-axis. This suggests a uniform motion along the

xx

-axis because the velocity remains constant with time. Secondly, the equation for

yy

is a second-degree polynomial in

tt

, which indicates a parabolic path. The presence of the

t2t^2

term (

8t28t^2

) signifies acceleration since the position along the

yy

-axis is changing at a rate that itself changes over time. The equation for

yy

can show two types of motion depending on the terms: If it was of the form

y=y0+vty = y_0 + vt

, it would indicate uniform motion. If it was of the form

y=y0+vt+12at2y = y_0 + vt + \frac{1}{2}at^2

, where

aa

would represent acceleration, it would indicate uniformly accelerated motion. The presence of the

8t28t^2

term here plays a similar role, indicating that the motion is uniformly accelerated in the

yy

-direction due to the constant acceleration implied by this term. Since the motion in the

yy

direction is determined by a quadratic equation, and the path of the particle depends on both the

xx

and

yy

coordinates, the motion of the particle is not along a straight line but rather follows a parabolic path due to the quadratic (second-degree) dependence on time in the

yy

-coordinate. Additionally, the acceleration is not changing with time, as deduced from the constant coefficient of the

t2t^2

term in the

yy

equation, indicating uniform acceleration.

Therefore, the motion is uniformly accelerated and follows a parabolic path.

Hence, the correct answer is: Option D: uniformly accelerated having motion along a parabolic path.

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