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Question: A particle is projected with a velocity $\vec{v} = (2\hat{i} + 3\hat{j})$ m/s in the presence of a u...

A particle is projected with a velocity v=(2i^+3j^)\vec{v} = (2\hat{i} + 3\hat{j}) m/s in the presence of a uniform acceleration a=(3i^4j^)\vec{a} = (-3\hat{i} - 4\hat{j}) m/s². The path of the particle will be

A

Straight line

B

Parabolic

C

Circular

D

Elliptical

Answer

Parabolic

Explanation

Solution

The position vector of a particle at time tt moving with initial velocity v0\vec{v}_0 and uniform acceleration a\vec{a} is given by:

r(t)=r(0)+v0t+12at2\vec{r}(t) = \vec{r}(0) + \vec{v}_0 t + \frac{1}{2}\vec{a}t^2

Let the initial position be the origin, r(0)=0\vec{r}(0) = \vec{0}. Given initial velocity v0=(2i^+3j^)\vec{v}_0 = (2\hat{i} + 3\hat{j}) m/s and uniform acceleration a=(3i^4j^)\vec{a} = (-3\hat{i} - 4\hat{j}) m/s². The position vector at time tt is:

r(t)=(2i^+3j^)t+12(3i^4j^)t2\vec{r}(t) = (2\hat{i} + 3\hat{j})t + \frac{1}{2}(-3\hat{i} - 4\hat{j})t^2 r(t)=(2t32t2)i^+(3t2t2)j^\vec{r}(t) = (2t - \frac{3}{2}t^2)\hat{i} + (3t - 2t^2)\hat{j}

Let the coordinates of the particle at time tt be (x(t),y(t))(x(t), y(t)).

x(t)=2t32t2x(t) = 2t - \frac{3}{2}t^2 y(t)=3t2t2y(t) = 3t - 2t^2

To find the path, we eliminate tt from these two equations. Multiply the first equation by 4 and the second by 3:

4x=8t6t24x = 8t - 6t^2 3y=9t6t23y = 9t - 6t^2

Subtract the first equation from the second:

3y4x=(9t6t2)(8t6t2)3y - 4x = (9t - 6t^2) - (8t - 6t^2) 3y4x=t3y - 4x = t

Now substitute this expression for tt back into either of the original equations. Using the equation for yy:

y=3(3y4x)2(3y4x)2y = 3(3y - 4x) - 2(3y - 4x)^2 y=9y12x2(9y224xy+16x2)y = 9y - 12x - 2(9y^2 - 24xy + 16x^2) y=9y12x18y2+48xy32x2y = 9y - 12x - 18y^2 + 48xy - 32x^2

Rearranging the terms to the left side:

32x2+18y248xy+12x+y9y=032x^2 + 18y^2 - 48xy + 12x + y - 9y = 0 32x2+18y248xy+12x8y=032x^2 + 18y^2 - 48xy + 12x - 8y = 0

This is a general second-degree equation in xx and yy of the form Ax2+Bxy+Cy2+Dx+Ey+F=0Ax^2 + Bxy + Cy^2 + Dx + Ey + F = 0. Here, A=32A = 32, B=48B = -48, C=18C = 18. The nature of the conic section is determined by the discriminant B24ACB^2 - 4AC.

B24AC=(48)24(32)(18)=23044(576)=23042304=0B^2 - 4AC = (-48)^2 - 4(32)(18) = 2304 - 4(576) = 2304 - 2304 = 0.

Since B24AC=0B^2 - 4AC = 0, the path is a parabola (or a degenerate case like parallel lines). In the case of motion under constant acceleration where the initial velocity is not parallel to the acceleration, the path is a parabola.

We can check if the initial velocity v0=(2,3)\vec{v}_0 = (2, 3) and acceleration a=(3,4)\vec{a} = (-3, -4) are parallel. Two vectors u\vec{u} and v\vec{v} are parallel if u=kv\vec{u} = k\vec{v} for some scalar kk. Is (2,3)=k(3,4)(2, 3) = k(-3, -4)?

2=3k    k=2/32 = -3k \implies k = -2/3 3=4k    k=3/43 = -4k \implies k = -3/4

Since the value of kk is not unique, the vectors are not parallel.

Therefore, the path is a parabola.