Solveeit Logo

Question

Question: If acc" of Particle is given by eq" $\vec{a}$ = (2x+1) m/s², where x Jis in mater (m). If at x=1m, v...

If acc" of Particle is given by eq" a\vec{a} = (2x+1) m/s², where x Jis in mater (m). If at x=1m, v=2m/sec. Then find v as f(x) (Junction of position)

a\vec{a} = 2x+1\int 2x + 1

Answer

v = 2x2+2x\sqrt{2x^2 + 2x}

Explanation

Solution

The acceleration of the particle is given by a=(2x+1)m/s2\vec{a} = (2x+1) \, \text{m/s}^2. Since the acceleration is given as a function of position xx, we use the relation a=vdvdxa = v \frac{dv}{dx}, where vv is the velocity of the particle.

So, we have: vdvdx=2x+1v \frac{dv}{dx} = 2x+1

This is a separable differential equation. We can separate the variables vv and xx: vdv=(2x+1)dxv \, dv = (2x+1) \, dx

Now, we integrate both sides. We are given that at x=1mx=1 \, \text{m}, the velocity v=2m/sv=2 \, \text{m/s}. We can use these as the limits of integration. Let the velocity at position xx be v(x)v(x). 2vvdv=1x(2x+1)dx\int_{2}^{v} v' \, dv' = \int_{1}^{x} (2x'+1) \, dx'

Integrating the left side: 2vvdv=[(v)22]2v=v22222=v222\int_{2}^{v} v' \, dv' = \left[ \frac{(v')^2}{2} \right]_{2}^{v} = \frac{v^2}{2} - \frac{2^2}{2} = \frac{v^2}{2} - 2.

Integrating the right side: 1x(2x+1)dx=[2(x)22+x]1x=[(x)2+x]1x\int_{1}^{x} (2x'+1) \, dx' = \left[ \frac{2(x')^2}{2} + x' \right]_{1}^{x} = \left[ (x')^2 + x' \right]_{1}^{x} =(x2+x)(12+1)=x2+x2= (x^2 + x) - (1^2 + 1) = x^2 + x - 2.

Equating the results from both sides: v222=x2+x2\frac{v^2}{2} - 2 = x^2 + x - 2

Add 2 to both sides: v22=x2+x\frac{v^2}{2} = x^2 + x

Multiply by 2: v2=2(x2+x)v^2 = 2(x^2 + x) v2=2x2+2xv^2 = 2x^2 + 2x

Taking the square root to find vv: v=±2x2+2xv = \pm \sqrt{2x^2 + 2x}

We are given the initial condition that at x=1x=1, v=2v=2. Let's check this condition with the derived equation: At x=1x=1, v2=2(12+1)=2(1+1)=2(2)=4v^2 = 2(1^2 + 1) = 2(1+1) = 2(2) = 4. So, v=±4=±2v = \pm \sqrt{4} = \pm 2. Since the given initial velocity is v=2v=2 (positive), we choose the positive root. v(x)=2x2+2xv(x) = \sqrt{2x^2 + 2x}.

This function represents the velocity as a function of position xx for the particle, consistent with the given acceleration and initial condition. The domain of xx for which the velocity is real is where 2x2+2x02x^2+2x \ge 0, which is 2x(x+1)02x(x+1) \ge 0, meaning x1x \le -1 or x0x \ge 0. The initial condition is at x=1x=1, which is in the region x0x \ge 0. Since the initial velocity is positive and the acceleration 2x+12x+1 is positive for x>1/2x > -1/2, the velocity will remain positive as the particle moves in the positive direction from x=1x=1.