• No results found

Motion in One Dimension

N/A
N/A
Protected

Academic year: 2021

Share "Motion in One Dimension"

Copied!
13
0
0

Loading.... (view fulltext now)

Full text

(1)

A t r u st e d n am e f o r Qu a l i t y E d u c at i o n … …

Motion in one Dimension

K

KIINNEEMMAATTIICCSSAANNDDDDYYNNAAMMIICCSS

The part of mechanics which deals with the description of the motion of an object without considering reason of the origin is called kinematics. Where as, the study of the motion of an object related to its cause is called dynamics. (i) Motion in one dimension: Motion of an object in a straight line is called one dimensional (1-D) motion. The position of a particle in one dimensional motion can be described by only one variable (say x). For a particle moving along a straight line (1-D motion) all the vector quantities such as position, velocity, displacement and acceleration have only one non-zero component.

(ii) Motion in two dimension: Motion of an object in a plane is called two dimensional (2-D) motions. For 2-D motion velocity or acceleration can be described by two components in any two mutually perpendicular directions in Cartesian coordinate system i.e. its position, velocity, displacement and acceleration can have two nonzero components.

(iii) Distance & Displacement:

Displacement: - The change in position of a body in a particular direction is known as displacement. It is a vector quantity and its unit in SI system is meter. The shortest distance between the initial and final positions of the object in a specified direction.

Distance: The total length of actual path traversed by a body in a certain interval of time is called distance. It is the actual path travelled by an object between its initial and final positions. It is a scalar quantity and its unit in SI is meter. Displacement may be positive, negative or zero but distance is always positive. If a particle moves in a straight line without change in its direction, the magnitude of displacement is equal to the distance travelled. Otherwise it is always less than it. Thus, Displacement  distance

Example 1 : What will be the distance and displacement while moving in a circle from A to B and then B to A as shown in adjoining figure?

A B

o

R R

Solution:

Physical quantity and direction Half cycle

AB or BA

Full cycle AA via B

Distance R 2R

Displacement 2R 0

Direction of displacement 1. AB, when particle moves from A to B.

2. BA, when particle moves from B to A.

(iv) Average Speed and Velocity: The average speed of a particle in a given interval of time is defined as the ratio of the distance travelled to the time taken while, average velocity is defined as the ratio of the displacement to the time taken.

If a particle moves from A to C through a path ABC. Then distance

 

Δs travelled is the actual path length ABC, while the displacement is,

C A

Δ r = r  - r

Thus, if the distance travelled is

 

Δs and displacement of a particle is Δr in a given time interval Δt then

A X C B YΔr  c r  A r

(2)

av av

Δs Δ r

v = A verage speed = and V = A verage velocity =

Δt Δt

 

(v) Instantaneous Speed and Velocity: Instantaneous speed and velocity are defined at a particular instant and are given by ,

Δt 0 Δt 0

Δs ds Δr dr v = lim = and V = lim =

Δt dt Δt dt

 

 



(vi) Average and Instantaneous Acceleration: Average acceleration is defined as the change in velocity

V



over a time interval t. Hence, aav V t   

The instantaneous acceleration of a particle is the rate at which its velocity is changing at that instant i.e.,

  ins a Δt 0 ΔV lim Δt     dV dt

Example 2 : A particle moves along a semi circle path A to B in a time T as shown in the following fig.

(a) Determine the average speed of the particle.

(b) Determine the average velocity of the particle. A B

o

Solution: (a) The average speed of the particle = distance

time  R T

(b) The average velocity of the particle= displacement

time  2R

T

E

EQQUUAATTIIOONNSSOOFFMMOOTTIIOONN

EQUATIONS OF MOTION FOR UNIFORM ACCELERATION

Consider a particle moving along a straight line with constant acceleration a. Let u be the initial velocity of the particle and v be the velocity at time t. By definition,

dv a dt   dv = a dt Integrating, v t t u 0 0 dv a dta dt

(a being a constant can be taken out of the integral)  v – u = at

 v = u + at …(i)

Further, v = dx

dt  dx = vdt

But, v = u + at,  dx = (u + at)dt Integrating within appropriate limits, we get,

s t 0 0 dx (uat)dt

 t t 0 0 s 0 u dt

a t dt

 1

2 2

s u(t 0) a t 0 2     t t 2 2 2 0 0 t 0 t dt t and t dt 2 2 2            

  1 2 s ut at 2   …(ii)

Again, going back to definition of a, we have, a dv dt 

Multiply and divide RHS of above equation by dx, we get, a dx dv dt dx           

(3)

 a vdv dx

  adv = adx

Integrating within appropriate limits, we get,

v s u 0 v dva dx

 s v 2 u 0 v ax 2   v2 u2 a(s 0) 2  2    2 2 v u 2as …(iii)

From (i) and (iii) we also conclude that, s u v t 2 

 

  …(iv)

Equation (iv) is a special equation, as we do not have a in this equation, but still it belongs to motion, which is uniformly accelerated.

To conclude, we again write the equation of motion for constant acceleration below. v = u + at ; s = ut + 1at2 2 ; 2 2 v u 2as; s u v t 2      EQUATION OF MOTION FOR VARIABLE ACCELERATION

Case I when acceleration a of the particle is a function of time i.e.

A = f(t)  dv f(t)

dt   dv = f(t)dt

Integrating both sides within suitable limits, we get,

v t u 0 dv f(t)dt

 v – u t 0 f(t)dt 

 v = u + t 0 f(t)dt

Case II When acceleration a of the particle is a function of distance i.e.

a = f(x)  dv dt = f(x)  dv dx dx dt = f(x)  vdv dx = f(x)  vdv = f(x)dx Integrating we get, v s u 0 vdv f(x)dx

 s 2 2 0 v u f(x)dx 2  2 

 s 2 2 0 v u 2 f(x)dx

Case III When acceleration a of the particle is a function of velocity i.e.,

a = f(v)  dv f(v) dt  Option 1 Option 2 dv dt f(v)  Integrating, t v 0 u dv dt f(v) 

v u dv t f(v)  

dv v f(v) dx  vdv dx f(v)   a vdv dx        Integrating, x v x0 u vdv dx f(v) 

0 v u vdv x x f(v)   

The displacement by the body in nth second is given by ,

(2

1)

2

 

n

a

s

u

n

Example 3: Choose the correct alternative(s)

The displacement of a particle moving along the x axis is given by x = a(t-1) + b(t-1)

Where a and b are constants; x is measured in meters and t is in second. The motion start at t = 0. (A) The initial velocity of the particle is a

(B) The acceleration of the particle is 2b (C) The initial velocity of the particle is (a + b)

(4)

(D) The particle starts its motion from the origin at t = 1sec.

Solution: x = a(t -1) + b(t -1) …(1)

dx

dt = a + b , so the initial velocity of the particle is (a + b)

putting t = 1sec.  x = 0 i.e the particle starts its motion from the origin at t = 1sec.Therefore C & D are the correct answers.

Example 4: A ball thrown up from the ground reaches a maximum height of 20m. Find (A) Its initial velocity

(B) the time taken to reach the highest point (C) the time at which it is 15m above the ground (D) its velocity just before hitting the ground (E) its displacement between 0.5 sec and 2.5 sec. Solution: (A) Using v2 = u2+2as for upward motion

0 = u2 + 2(-9.8)  (20)  u= 19.8 m/s (B) 0 19.8 2.02 sec 9.8     v - u t = a

(C) using s = ut + ½gt2 15 = 19.8t - ½ 9.8 t2  t= 1.01 sec & 3.303sec.

There are two solutions because At t = 1.01 ball is going up and at t= 3.303sec it is coming down.

(D) displacement is zero for the complete up-down trip. v2= u2+ 2 a (0) (by using v2= u2+ 2as)  v2

= u2  v = u = –19.8 m/s

(E) height at t = 0.5 sec. can be calculate using s = ut + ½ at2 y1= 19.8 (0.5) – 4.9 (0.5) 2 = 8.68 m height at t = 2.53 is, y2= 19.8 (2.5) – 4.9 (2.5) 2 = 18.9 m displacement = y2– y1= 18.9 m – 8.68 m = 10.2 m

Common Error in kinematics

In using kinematical eqn. (1D), S = ut + at1 2

2

Here 'S' in the displacement i.e. s = xf - xi. Its common error for the student to think that displacement and distance are the same.

Example 5: A ball is projected with a velocity of 20 m/s vertically. Find the distance travelled in first three second. (use g = 10m/sec2 )

Solution: Here the problem is to find the distance. We can calculate that the direction of ball is changes at t = 2s. (From v = u + at, since v = 0 at highest point therefore 0=20 - 10t  t = 2s)

Distance travelled in first two seconds

( Distance = Displacement, because velocity does not change direction in one dimension)

1

1

S = 20× 2 - ×10 × 4

2 = 40 – 20 = 20 m (upward)

Distance travelled in next one second ,

downward

2

1

S = - ×10 ×1 = -5m 2

So total distance travelled by the ball in first three seconds = 20 +5 = 25m

Example 6: A particle moves along the x-axis according to x = 4t – t2. Find the distance travelled from t = 0s to t = 3s.

Solution: The direction of velocity will change when V = 0 at t = 2 sec. Distance = 3 0

vdt= 1 2 3 0 1 2 (42 )  (42 )  (42 )

t dt

t dt

t dt = 3+1+ 1 =5 meter

Example 7: A particle moving with uniform acceleration from A to B along a straight line has velocities v1and v2at A and B respectively. If C

is the mid point between A and B then determine the velocity of the particle at C.

A C B

v1 v2

(5)

V2 = v1 2

+ 2a (x/2)

Where a is the acceleration of the particle; i.e.  

 

2 1

v v

t

t is the time taken by the particle to travel from A to B and x is the total distance between A and B,

i.e. 1 2 2    v v x t 1 2 2        v v t  2 1     v v t Thus, V 2 –v12 2 2 1 2 2   v v

Example 8: A particle travels according to the equation a A Bv where

a

is the acceleration. A and B are constants,

v

is the velocity of the particle. Find its velocity as a function of time. Also find terminal velocity. Solution: dv A B dt    or

V t e 0 0 0 dv 1 dt log A B t A B B         

or loge A B Bt A    or A B AeBt or A

1 e Bt

B        

At terminal velocity, acceleration = 0, that is,  t A / B

X

X

T

T

,

,

V

V

T

T

&

&

A

A

T

T

G

G

R

R

A

A

P

P

H

H

S

S

F

F

O

O

R

R

M

M

O

O

T

T

I

I

O

O

N

N

I

I

N

N

O

O

N

N

E

E

D

D

I

I

M

M

E

E

N

N

S

S

I

I

O

O

N

N

(i) Variation of displacement (x), velocity (v) and acceleration (a) with respect to time for different types of motion.

Displacement(x) Velocity(v) Acceleration (a)

a. At rest x t O x=constant v t O a t O b. Motion with constant velocity x t O x0 x = x0+ v0t +x0t2 v t O v0v = constant a t O c. Motion with constant acceleration x t O x = v0t +(1/2)a0t2 v t O v = v0+a0t v0 a t O a0 a = constant d. Motion with constant deceleration x t O x = v0t -(1/2)a0t2 v t O v0 a t O a0 a = constant

(ii) Displacement calculation from Velocity - Time Graphs: The displacement during an interval

between time tiand tfis the area bounded by the velocity curve and the two vertical lines t = tiand t = tf, as

(6)

t O v1 v v2 v3 v4 1 t  t2t3t4 f t i t

(a) For each segment of motion, the velocity is

constant. The displacement xiduring the i th

interval is the area vi ti. So the total displacement is x

x = v1t1+ v2t2+ v3t3 + v4t4

 x

v tii

(b) When v vs. t graph is a smooth complex curve.

Area bounded by the curve and time axis between t=ti and t=tf is the displacement. The area under

the curve may be obtained by using integration.

(iii) Velocity calculation from Acceleration - time Graphs: Given an acceleration–versus–time graph,

the change in velocity between t = tiand t = tfis the area bounded by the acceleration curve and the vertical

lines t = tiand t = tf t O a ti tf a0

(a) When the area under the a vs t is a smooth

curve then the change in velocity v a t 0

(b) When a vs t graph is a complex curve, the area

under the curve may be obtained by using integration

Example 9: The velocity-time graph of a particle moving along a

straight line is shown in following figure.

(i) If the particle starts its motion from x = –4m, then draw the (a–t) and (x–t) graphs. (ii) Find the displacement of the particle at t = 3 s

t O v 2 4 4 m/s Time v e lo c it y Solution: (i) t(s) O a 1 +2 2 m/s2 -2 3 4 t(s) O x 2 -4 4 x(m) +4 (ii) 3 0 [Area of v-t graph] 0     t t x x 1 4 2 4 (2)(4) (3 2) or 3 2 2            x x m

(7)

+10 0 -10 5 10 15 t(s) a(ms-2)

Solution: Velocity is the area under

a t

curve, thus at the end

of 5s, velocity v50ms1. Since there is no acceleration in the interval (5 -10 s), therefore velocity remains constant, that is, 50ms1. In the interval (10 – 15 s) the particle is retarded (Area = -50). Thus, we get the (v – t) curve as shown in figure (a) Hence particle

comes to rest. v t

To draw

s t

graph [Fig (b)]. We take help of

v t

graph. Area under

v t

curve is the distance travelled. Distance moved in

0 5

50 5 125 2   s ism Distance moved in

5 10 s is

5 50 250m Distance moved in

10 15

50 5 125 2   s ism 5 0 0 5 1 0 1 5 t s ( m ) 0 ( s - t ) c u r v e 1 2 5 3 7 5

Example 11: A ball drops from a height 19.6 m above the ground, it rebounds and rises to the same

height. Plot

v t

and

x t

graphs

Solution: 1 2 2

x = gt 19.6 2 9.8 t

2 Þ ´ = or t ¾ 2s

This is the time for the ball to come to the ground.

-19.6 19.6 0 1 2 3 4 t v(ms-1) 19.6 0 1 2 3 4 t x(m)

Velocity – Time graph Distance –Time graph

Example 12: Plot

v - t

and

x - t

graph for the given

a - t

graph.

Solution: To plot the

v t

graph we can see from the (a-t)

graph, that

                 

5 2 5 5 1 0 0 0 1 a 2 t 0 t 5 s 2 t v a d t 2 td t 2 5 m s 2 v u a t 5 s t 1 0 s 2 5 1 0 5 7 5 m s a t th e e n d o f 1 0 s 0 0 5 10 10 a(ms-2) t

(8)

For

x t

graph,

(

)

5 3 5 0 0 t 125 x v.dt m 0 t 5s 3 3 =

ò

= = < <

x

= area under

v t

curve (5s < t < 10 s) = 250 m.

Example 13: A particle starts from rest with acceleration

for some time and after achieving a

maximum velocity starts retarding at rate

and finally comes to rest. If total time taken is t then Determine (a) maximum velocity (b) total distance travelled.

(A)

2 , t t





 

 

 (B)

2 , 2 t t





 

 

 (C)

2 , 2 2 t t

 

 

(D)

 

2 , 2 t t

 

 

Solution: (B) Let the particle accelerate for a time t then maximum, velocity v

t1

t1 t-t1

 

v

t

Since it retards at a rate

and finally comes to rest therefore 0

t1

tt1

Or t1

t vmax



t

 

 

  

 

Distance travelled = area under (v -t) graph

max. 1 2v total time

2 1 t= 2 2 t t





 

 

   

Example 14: The displacement of a particle moving in one dimension is given by tx3 where x

is in meter and t in second. The displacement, when the velocity is zero is (A) 3 m (B) 1 m (C) 1.8 m (D) None of these

Solution: (D) x

(

t 3

)

2 and dx 2 t

(

3

)

dt = - = -dx v 0 when t 3 dt = = =

(

)

2 x= 3- 3 =0

Example 15: A body is moved along a straight line path by a machine delivering constant power. The

(9)

(A) 3 2

t

(B) 1 4

t

(C) 1 2

t

(D) 3 4

t

Solution: Power PF.vmdVv vdv

P.dt dt m 2 v P or t C when t 0, v 0 C=0 2 =m + = = \ 2Pt dx 2Pt or v or m dt m = =  

1 3 2 2 2P dx t dt or x t

(10)

A

A

S

S

S

S

I

I

G

G

N

N

M

M

E

E

N

N

T

T

LEVEL - I

1. The motion of a body is given by the equation d (t) 6 3 (t) dt

u

= - u

Where ( ) t at time t is in ms–1 and t is in seconds. If the body was at rest at t = 0, test the correctness of the following results

(A) The terminal speed is 2 ms –1.

(B) The magnitude of the initial acceleration is 8 ms2. (C) The speed varies with time as (t) 2(1 e-3t)

u =

-(D) The speed variation is 2 ms–1when the acceleration is half the initial value.

2. A driver applies brakes to the vehicle on seeing traffic signal 400 m ahead. At the time of applying the brakes vehicle was moving with 15 ms-1and then starts retarding with 0.3 ms-2. The distance of vehicle after 1 min from the traffic light:

(A) 25m (B) 375m (C) 360m (D) 40m

3. A particle is moving along a circular path of radius 5m and with uniform speed 5 m/s. What will be the average acceleration when the particle completes half revolution?

(A) zero (B) 10 m/s2 (C) 10 m/s2 (D) 10/m/s2

4. Which of the following graph correctly represents velocity-time relationship for a particle released from rest to fall freely under gravity?

v t v t v t v t (A) (B) (C) (D)

5. A bus accelerate uniformly from rest and acquires a speed of 36 km/hour in 10 seconds. The acceleration is

(A) 1000 m/sec2 (B) 1 m/sec2 (C) 100 m/sec2 (D) 10 m/sec2

6. A stone is thrown vertically up from the ground. It reaches a maximum height of 50 meters in 10 sec. After what time it will reach the ground from the maximum height position?

(A) 1.2 sec (B) 5 sec (C) 10 sec (D) 25 sec

7. A body thrown up with a velocity reaches a maximum height of 50 meters. Another body with double the mass thrown up, with double the initial velocity will reach a maximum height of

(A) 100 m (B) 200 m (C) 10 m (D) 400 m

8. The reaction time for a car driver is 0.9 sec. If the car travelling initially with 36 Km/hr is stopped by the driver in two seconds after observing a signal by the deceleration of 5 m/s2, the total distance traveled by the car before coming to rest is

-(A) 19 m (B) 9 m (C) 10 m (D) 28 m

9. A car starts from rest. Attains a velocity of 36 km/h with an acceleration of 0.2 m/s2, travels 9 km with this uniform velocity and then comes to halt with a uniform deceleration of 0.1 m/s2. The total time of travel of the car is

(A) 1050 s (B) 1000 s (C) 950 s (D) 900 s

10. A car travelling on a straight track moves with uniform velocity V1 for some time and with uniform

velocity V2for next equal time, the average velocity is given by

(A) V V1 2 (B) V V1 2 2 (C) 1 1 2 1 1 V V         (D) 1 1 2 1 1 2 V V        

11. A lift is moving with a retardation of 5 m/s2. The percentage change in the weight of person in the lift is (g = 10 m/s2)

(A) 100 (B) 25 (C) 50 (D) 75

12. The distances traveled by a body starting from rest and travelling with uniform acceleration, in successive intervals of time of equal duration will be in the ratio

(11)

(A) 1 : 2 : 3 (B) 1 : 2 : 4 (C) 1 : 3 : 5 (D) 1 : 5 : 9

13. The average velocity of a body moving with uniform acceleration after travelling a distance of 3.06 m is 0.34 m/s–1. If the change in velocity of the body is 0.18 ms–1 during this time its uniform acceleration is.

(A) 0.01 m/s2 (B) 0.02 m/s2 (C) 0.03 m/s2 (D) 0.04 m/s2

14. Equation of position (x) with time (t) is given by equation x = 3t2+ 7t2 + 5t + 8m. The acceleration at time t = 1 sec. is :

(A) 18 m/sec2 (B) 32 m/sec2 (C) Zero (D) 14 m/sec2

15. A man slides down an inclined plane and drops a bag from the position to the ground. If velocities of man and bag on reaching the ground are vMand vB respectively then:

(A) vMvB (B) vMvB (C) vMvB (D) depend on weight

16. One car moving on a straight road covers one third of the distance with 20 km/hr and the rest with 60 km/hr. The Average speed is

(A) 40 km/hr (B) 80 km/hr (C) 462km / hr

3 (D) 36 km/hr

17. A particle covers 50m. distance with 40 kmph and rest half distance with 60 kmpl then the average speed of car is :

(A) 100 m (B) 150 m (C) 200 m (D) 250 m

18. A car travels half distance with 40 kmph and rest half distance with 60 kmph then the average speed of car is :

(A) 40 kmph (B) 48 kmph (C) 52 kmph (D) 60 kmph

19. A particle is moving east-wards with a velocity of 15 m/s. In a time of 10 seconds, the velocity changes to 15 m/s north-wards. Average acceleration during this time is, in m/s2

(A) 3

2 north-east (B) 3 2 north-east (C) 3

2 north-west (D) 3 2 north-west

20. A car starts from rest and travels with uniform acceleration  for some time and then with uniform retardation  and comes to rest. If the total travel time of the car is 't', the maximum velocity attained by it is given by (A) .t ( )     (B) 2 1 .t 2 ( )     (C) ( ).t     (D) 2 1 .t 2 ( )    

(12)

LEVEL - II

1. Water drops fall from a tap on to the floor 5.0 m below at regular intervals of time, the first drop striking the floor when the fifth drop begins to fall. The height at which the third drop will be from ground, at that instant when first drop strikes the ground, will be, taking g = 10.0 m/sec2.

(A) 1.25 m (B) 2.15 m (C) 2.75 m (D) 3.75 m

2. A stone is dropped freely, while another is thrown vertically downward with an initial velocity of 2 ms2 from the same point, simultaneously. The time required by them to have a distance of separation 22 m between them is

(A) 11 sec. (B) 5.5 sec. (C) 44 sec. (D) 22 sec.

3. A body is thrown vertically upwards with an initial velocity u reaches maximum height in 6 seconds. The ratio of distance traveled by the body in the first, second and seventh second is :

(A) 1 : 1 (B) 11 : 1 (C) 1 : 2 (D) 1 : 11

4. A particle travels 10 m in first 5 sec and 10 m in next 3 sec. assuming constant acceleration what is the distance traveled in next 2 sec.

(A) 8.3 m (B) 9.3 m (C) 10.3 m (D) None

5. Acceleration of a particle changes when :

(A) Direction of velocity changes (B) Magnitude of velocity changes

(C) both of above (D) speed changes

6. The relation 3t 3x6 describes the displacement of a particle in one direction where x is in meters and t in sec. The displacement, when velocity is zero, is

(A) 24 m (B) 12 m (C) 5 m (D) zero

7. The displacement 'x' of a particle moving along a straight line at time t is given by xa0a t1 a t2 2 what is the acceleration of the particle?

(A) a1 (B) a2 (C) 2a2 (D) 3a2

8. A body starts from rest and has an acceleration 20 cm/sec2. What is the distance covered by the

body in first 8 sec ?

(A) 160 cm (B) 640 cm (C) 1280 cm (D) 1640 cm

9. Pick up the correct statements:

(A) Area under a-t graph gives velocity

(B) Area under a-t graph gives change in velocity

(C) Path of projectile as seen by another projectile is a parabola,

(D) A body, whatever be its motion, is always at rest in a frame of reference fixed to the body itself.

10. A body is moving in a circle at a uniform speed

. What is the magnitude of the change in velocity when the radius vector describes an angle :

(A) cos (B) 2 cos

2        (C) sin (D) 2 sin 2       

11. A bicyclist encounter a series of hills uphill whose speed is always v1 and down hill speed is always

v2. The total distance travelled is , with uphill and downhill portions of equal length. The cyclist's

average speed is:

(A) 2 v v12 (B) 2 1 2 2 2 1 v v v v   (C) 2 1 2 1 v v v v  (D) 1 2 2 1 v v v v 2 

12. Choose the wrong statement:

(A) Zero velocity of a particle does not necessarily mean that its acceleration is zero. (B) Zero acceleration of a particle does not necessarily mean that its velocity is zero. (C) If the speed of a particle is constant, its acceleration must be zero.

(D) None of these

13. Displacement (x) of a particle is related to time (t) as x = at + bt2 – ct3 where a, b and c are constants of motion. The velocity of the particle when its acceleration is zero is given by:

(A) 2 b a c  (B) 2 2 b a c  (C) 2 3 b a c  (D) 2 4 b a c

(13)

14. A particle moving in a straight line covers half the distance with speed of 3 m/s. The other half of the distance is covered in two equal time intervals with speed of 4.5 m/s and 7.5 m/s respectively. The average speed of the particle during this motion is

(A) 4.0 m/s (B) 5.0 m/s (C) 5.5 m/s (D) 4.8 m/s

15. The acceleration of a particle is increasing linearly with time t as bt. The particle starts from the origin with an initial velocity v0. The distance travelled by the particle in time t will be

(A) 2 0 1 v t bt 3 + (B) 3 0 1 v t bt 3 + (C) 3 0 1 v t bt 6 + (D) 2 0 1 v t bt 2 +

16. The motion of a body is given by the equation dv(t) 6.0 3v(t)

dt = - . where v(t) is speed in m/s and t in sec. If body was at rest at t = 0

(A) The terminal speed is 2.0 m/s

(B) The speed varies with the time as v(t) = 2(1 – e–3t) m/s

(C) The speed is 0.1 m/s when the acceleration is half the initial value (D) The magnitude of the initial acceleration is 6.0 m/s2

17. A particle starts from rest. Its acceleration (a) versus time (t) is as shown in the figure. The maximum speed of the particle will be

(A) 110 m/s (B) 55 m/s (C) 550 m/s (D) 660 m/s

18. If a ball is thrown vertically upwards with speed u, the distance covered during the last t seconds of its ascent is (A) 1gt2 2 (B) 2 1 ut gt 2 - (C) (u – gt)t (D) ut d

19. A particle is acted upon by a force of constant magnitude which is always perpendicular to the velocity of the particle. The motion of the particle takes place in a plane. It follows that

(A) Velocity is constant (B) Acceleration is constant (C) Kinetic energy is variable (D) It moves in a circular path

20. The variation of velocity of a particle with time moving along a straight line is illustrated in the following figure. The distance traveled by the particle in four second is

(A) 60 m (B) 55 m (C) 25 m (D) 30 m

References

Related documents

The essays by Nadine Boljkovac and Felicity Colman examine the ability of cinema and video to go beyond representation by extracting affect from both subjective interiority and

Hitlerove uslove predsedniku. februara austrijska vlada je po čela da ispunjava nemačke uslove. Ali Hitler je naumio da u potpunosti ostvari svoje ciljeve. U govoru pred

6 EBITDA was impacted by extraordinary costs associated with the acquisition of Navitaire incurred in 2015 (€6.7 million) and with the acquisition of i:FAO in 2014 (€1.6

This qualitative study investigates knowledge transfer in college students whose high school Advanced Placement (AP) or dual credit (DC) English courses enabled them to opt out of

For the prediction of the trainings response with MRI- and gene-based biological factors, we found that patients with larger left entorhinal cortex volume improved significantly more

decomposition. These suites of soil properties characterize the landscape positions of agricultural regions, yet their effect on root biomass and decomposition has not been

Study of ferroelectric/dielectric multilayers for tunable stub resonator applications at microwaves.. Yonathan Corredores, Arnaud Le Febvrier, Xavier Castel, Ronan Sauleau,

The molecular junction conductance of a series of oligophenyls was successfully measured, highlighting the potential of an all-carbon based approach for the fabrication