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Laws of Motion question

2020 · 6 Sep · Shift 2 · Q48
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  5. /2020 · 6 Sep · Shift 2 · Q48

Laws of Motion question

2020 · 6 Sep · Shift 2 · Q48

JEE MainPhysicsLaws of MotionMCQ+4 / −1
A particle moving in the xy plane experiences a velocity dependent force F→=k(vyi^+vxj^)\overrightarrow F = k\left( {{v_y}\widehat i + {v_x}\widehat j} \right)F=k(vy​i+vx​j​), where vx and vy are the x and y components of its velocity v→\overrightarrow vv. If a→\overrightarrow aa is the acceleration of the particle, then which of the following statements is true for the particle?
  1. A
    kinetic energy of particle is constant in time
  2. B
    quantity v→×a→\overrightarrow v \times \overrightarrow av×a is constant in time
  3. C
    quantity v→.a→\overrightarrow v .\overrightarrow av.a is constant in time
  4. D
    F→\overrightarrow FF arises due to a magnetic field
View written solutionFree

Correct answer: B

  1. Given force law

The force is

F⃗=k (vyi^+vxj^)\vec F = k\,(v_y\hat i + v_x\hat j)F=k(vy​i^+vx​j^​)

So the acceleration is

a⃗=F⃗m=km(vyi^+vxj^)\vec a = \frac{\vec F}{m} = \frac{k}{m}(v_y\hat i + v_x\hat j)a=mF​=mk​(vy​i^+vx​j^​)

Hence,

ax=kmvy,ay=kmvxa_x = \frac{k}{m}v_y, \qquad a_y = \frac{k}{m}v_xax​=mk​vy​,ay​=mk​vx​
  1. Check option A: Is kinetic energy constant?

Rate of change of kinetic energy is

ddt(12mv2)=F⃗⋅v⃗\frac{d}{dt}\left(\frac12 mv^2\right)= \vec F\cdot \vec vdtd​(21​mv2)=F⋅v

Now,

F⃗⋅v⃗=k(vyi^+vxj^)⋅(vxi^+vyj^)\vec F\cdot \vec v = k(v_y\hat i + v_x\hat j)\cdot (v_x\hat i + v_y\hat j)F⋅v=k(vy​i^+vx​j^​)⋅(vx​i^+vy​j^​) =k(vxvy+vyvx)=2kvxvy= k(v_xv_y + v_yv_x)=2kv_xv_y=k(vx​vy​+vy​vx​)=2kvx​vy​

This is not zero in general, so kinetic energy is not constant.

So, A is false.

  1. Check option C: Is v⃗⋅a⃗\vec v\cdot \vec av⋅a constant?

We have

v⃗⋅a⃗=(vxi^+vyj^)⋅km(vyi^+vxj^)\vec v\cdot \vec a = (v_x\hat i+v_y\hat j)\cdot \frac{k}{m}(v_y\hat i+v_x\hat j)v⋅a=(vx​i^+vy​j^​)⋅mk​(vy​i^+vx​j^​) =km(vxvy+vyvx)=2kmvxvy= \frac{k}{m}(v_xv_y+v_yv_x)=\frac{2k}{m}v_xv_y=mk​(vx​vy​+vy​vx​)=m2k​vx​vy​

This is generally not constant because vxv_xvx​ and vyv_yvy​ change with time.

So, C is false.

  1. Check option B: Is v⃗×a⃗\vec v\times \vec av×a constant?

Since motion is in the xyxyxy-plane, v⃗×a⃗\vec v\times \vec av×a is along k^\hat kk^:

v⃗×a⃗=∣i^j^k^vxvy0axay0∣=(vxay−vyax)k^\vec v\times \vec a = \begin{vmatrix} \hat i & \hat j & \hat k\\ v_x & v_y & 0\\ a_x & a_y & 0 \end{vmatrix} = (v_xa_y-v_ya_x)\hat kv×a=​i^vx​ax​​j^​vy​ay​​k^00​​=(vx​ay​−vy​ax​)k^

Substitute

ax=kmvy,ay=kmvxa_x=\frac{k}{m}v_y,\qquad a_y=\frac{k}{m}v_xax​=mk​vy​,ay​=mk​vx​

Then,

vxay−vyax=vx(kmvx)−vy(kmvy)v_xa_y-v_ya_x = v_x\left(\frac{k}{m}v_x\right)-v_y\left(\frac{k}{m}v_y\right)vx​ay​−vy​ax​=vx​(mk​vx​)−vy​(mk​vy​) =km(vx2−vy2)=\frac{k}{m}(v_x^2-v_y^2)=mk​(vx2​−vy2​)

So,

v⃗×a⃗=km(vx2−vy2)k^\vec v\times \vec a = \frac{k}{m}(v_x^2-v_y^2)\hat kv×a=mk​(vx2​−vy2​)k^

Now check whether vx2−vy2v_x^2-v_y^2vx2​−vy2​ is constant:

ddt(vx2−vy2)=2vxv˙x−2vyv˙y\frac{d}{dt}(v_x^2-v_y^2)=2v_x\dot v_x-2v_y\dot v_ydtd​(vx2​−vy2​)=2vx​v˙x​−2vy​v˙y​

Using

v˙x=ax=kmvy,v˙y=ay=kmvx\dot v_x=a_x=\frac{k}{m}v_y,\qquad \dot v_y=a_y=\frac{k}{m}v_xv˙x​=ax​=mk​vy​,v˙y​=ay​=mk​vx​

we get

ddt(vx2−vy2)=2vxkmvy−2vykmvx=0\frac{d}{dt}(v_x^2-v_y^2)=2v_x\frac{k}{m}v_y-2v_y\frac{k}{m}v_x=0dtd​(vx2​−vy2​)=2vx​mk​vy​−2vy​mk​vx​=0

Hence vx2−vy2v_x^2-v_y^2vx2​−vy2​ is constant, so

v⃗×a⃗\vec v\times \vec av×a

is constant in time.

So, B is true.

  1. Check option D: Does this force arise due to a magnetic field?

Magnetic force is always of the form

F⃗=q(v⃗×B⃗)\vec F = q(\vec v\times \vec B)F=q(v×B)

which is always perpendicular to v⃗\vec vv, so

F⃗⋅v⃗=0\vec F\cdot \vec v = 0F⋅v=0

But here,

F⃗⋅v⃗=2kvxvy\vec F\cdot \vec v = 2kv_xv_yF⋅v=2kvx​vy​

which is not zero in general. Therefore this force cannot be purely magnetic.

So, D is false.

  1. Final answer

The correct option is:

B\boxed{\text{B}}B​
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