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Magnetism question

2017 · Shift 2 · Q40
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  5. /2017 · Shift 2 · Q40

Magnetism question

2017 · Shift 2 · Q40

JEE AdvancedPhysicsMagnetismMultiple correct+4 / −1
A uniform magnetic field BBB exist in the region between x=0x=0x=0 and x=3R2x = {{3R} \over 2}x=23R​(region 222 in the figure) pointing normally into the plane of the paper. A particle with charge +Q+Q+Q and momentum ppp directed along xxx-axis enters region 222 from region 111 at point P1(y)=−R).{P_1}\left( y \right) = -R).P1​(y)=−R). Which of the following option(s) is/are correct? JEE Advanced 2017 Paper 2 Offline Physics - Magnetism Question 40 English
  1. A
    For B>23pQRB \gt {2 \over 3}{p \over {QR}}B>32​QRp​ the particle well re-enter region 111
  2. B
    For B=813pQR,B = {8 \over {13}}{p \over {QR}},B=138​QRp​, the particle will enter region 333 through the point P2{P_2}P2​ on xxx-axis
  3. C
    When the particle re-enters region 111 through the longest possible path in region 2,2,2, the magnitude of the change in its linear momentum between point P1{P_1}P1​ and the farthest point from yyy-axis is p/2p/\sqrt 2p/2​
  4. D
    For a fixed B,B,B, particles of same charge QQQ and same velocity v,v,v, the distance between the point P1{P_1}P1​ and the point of re-entry into region 111 is inversely proportional to the mass of the particle
View written solutionFree

Correct answer: A, B

  1. Radius of motion inside the magnetic field

A charged particle entering a uniform magnetic field normally moves along a circular arc of radius

r=pQB.r=\frac{p}{QB}.r=QBp​.

Here the field exists only in the strip

0≤x≤3R2,0\le x\le \frac{3R}{2},0≤x≤23R​,

and the particle enters at

P1=(0,−R)P_1=(0,-R)P1​=(0,−R)

with momentum along +x+x+x.

Since B⃗\vec BB is into the plane and charge is +Q+Q+Q, the magnetic force is upward at entry, so the center of the circular path lies vertically above P1P_1P1​ by distance rrr.

Hence the circle is

x2+(y+r+R)2=r2.x^2+(y+r+R)^2=r^2.x2+(y+r+R)2=r2.

So the center is

C=(0, −R+r).C=(0,\,-R+r).C=(0,−R+r).
  1. Condition for re-entering region 1

The particle re-enters region 1 if it comes back to the line x=0x=0x=0 after entering region 2.

For the circle, intersections with x=0x=0x=0 are obtained from

(y+r+R)2=r2(y+r+R)^2=r^2(y+r+R)2=r2

which gives

y=−Randy=−R−2r.y=-R \quad \text{and} \quad y=-R-2r.y=−Randy=−R−2r.

Thus the second intersection always exists mathematically, and the particle returns to region 1 after tracing the right semicircle provided it does not leave through the boundary x=3R2x=\frac{3R}{2}x=23R​ before that.

The maximum xxx-coordinate on the circular path is x=rx=rx=r.

So:

  • if r<3R2r<\frac{3R}{2}r<23R​, the whole relevant arc lies inside region 2 and it returns to region 1;
  • if r=3R2r=\frac{3R}{2}r=23R​, it just touches the boundary;
  • if r>3R2r>\frac{3R}{2}r>23R​, it exits into region 3 before returning to region 1.

Therefore re-entry into region 1 occurs when

r<3R2.r<\frac{3R}{2}.r<23R​.

Using r=pQBr=\frac{p}{QB}r=QBp​,

pQB<3R2⇒B>23pQR.\frac{p}{QB}<\frac{3R}{2} \quad\Rightarrow\quad B>\frac{2}{3}\frac{p}{QR}.QBp​<23R​⇒B>32​QRp​.

So Option A is correct.


  1. Check whether for B=813pQRB=\frac{8}{13}\frac{p}{QR}B=138​QRp​ the particle enters region 3 through the point P2P_2P2​ on the xxx-axis

Given

B=813pQRB=\frac{8}{13}\frac{p}{QR}B=138​QRp​

so

r=pQB=pQ(813pQR)=13R8.r=\frac{p}{QB}=\frac{p}{Q\left(\frac{8}{13}\frac{p}{QR}\right)}=\frac{13R}{8}.r=QBp​=Q(138​QRp​)p​=813R​.

Since

13R8=1.625R>3R2=1.5R,\frac{13R}{8}=1.625R>\frac{3R}{2}=1.5R,813R​=1.625R>23R​=1.5R,

particle indeed reaches the boundary x=3R2x=\frac{3R}{2}x=23R​ and enters region 3.

Now check whether this happens at the xxx-axis, i.e. at y=0y=0y=0.

Equation of path:

x2+(y+r+R)2=r2.x^2+(y+r+R)^2=r^2.x2+(y+r+R)2=r2.

At boundary x=3R2x=\frac{3R}{2}x=23R​,

(3R2)2+(y+r+R)2=r2.\left(\frac{3R}{2}\right)^2+(y+r+R)^2=r^2.(23R​)2+(y+r+R)2=r2.

If crossing point is on xxx-axis, set y=0y=0y=0:

(3R2)2+(r+R)2=r2.\left(\frac{3R}{2}\right)^2+(r+R)^2=r^2.(23R​)2+(r+R)2=r2.

This is not the correct sign because from geometry the relevant point on the circle should satisfy

y=−R+r−r2−x2.y=-R+r-\sqrt{r^2-x^2}.y=−R+r−r2−x2​.

So for y=0y=0y=0,

0=−R+r−r2−x20=-R+r-\sqrt{r^2-x^2}0=−R+r−r2−x2​

with x=3R2x=\frac{3R}{2}x=23R​,

r2−(3R2)2=r−R.\sqrt{r^2-\left(\frac{3R}{2}\right)^2}=r-R.r2−(23R​)2​=r−R.

Squaring,

r2−9R24=r2−2rR+R2r^2-\frac{9R^2}{4}=r^2-2rR+R^2r2−49R2​=r2−2rR+R2 2rR=13R242rR=\frac{13R^2}{4}2rR=413R2​ r=13R8.r=\frac{13R}{8}.r=813R​.

This is exactly the obtained radius. Hence the particle crosses into region 3 at

(3R2,0)=P2.\left(\frac{3R}{2},0\right)=P_2.(23R​,0)=P2​.

So Option B is correct.


  1. Check Option C

The longest possible path in region 2 while still re-entering region 1 occurs for the limiting case

r=3R2r=\frac{3R}{2}r=23R​

(when the path just touches the boundary x=3R2x=\frac{3R}{2}x=23R​ before returning).

The farthest point from the yyy-axis is then the rightmost point of the circle:

(x,y)=(r, −R+r)=(3R2,R2).(x,y)=\left(r,\,-R+r\right)=\left(\frac{3R}{2},\frac{R}{2}\right).(x,y)=(r,−R+r)=(23R​,2R​).

At this rightmost point, the momentum has turned by 90∘90^\circ90∘ from its initial direction (initially along +x+x+x, there it is along −y-y−y).

So the magnitude of change in momentum is

∣Δp⃗∣=p2+p2=p2.|\Delta \vec p|=\sqrt{p^2+p^2}=p\sqrt2.∣Δp​∣=p2+p2​=p2​.

Not p2\frac{p}{\sqrt2}2​p​.

Hence Option C is false.


  1. Check Option D

For fixed BBB, same charge QQQ, same velocity vvv:

p=mv,r=pQB=mvQB.p=mv, \qquad r=\frac{p}{QB}=\frac{mv}{QB}.p=mv,r=QBp​=QBmv​.

So r∝mr\propto mr∝m.

If the particle re-enters region 1, the second intersection with x=0x=0x=0 is at

y=−R−2r.y=-R-2r.y=−R−2r.

Thus distance between entry and re-entry points is

2r=2mvQB,2r=2\frac{mv}{QB},2r=2QBmv​,

which is directly proportional to mass, not inversely proportional.

Hence Option D is false.


  1. Final conclusion

Correct options are:

A, B\boxed{A,\ B}A, B​

These match the stored correct answer.

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