A mass m is at rest on a horizontal frictionless surface at t=0. then a constant force f0 acts on it for a time t0. suddenly the force doubles to 2f0 and remains constant until t=2t0. part a determine the total distance traveled from t=0 to t=2t0.

Respuesta :

The total distance travel by the object is 2.5(F0/m)(t0)^2

Since constant force is applied on the object so we can apply the equation of linear motion.

According to law of inertia

F=ma

therfore for the time period t=0 to t_o the acceleration of the object is

a=F0/m

And the velocity of the object after t0 sec is calculated by the first equation of motion

v=u+at

since the initial velocity of the object is 0, therefore the velocity of the object after t0 sec is

v=(F0/m)*t0

and the distance cover by the object during t0 sec is calculated by the second equation of motion

s1=ut+0.5at^2

Plugging the values

s1=0.5(F0/m)(t0)^2

Now the acceleration of the object during 2t0 sec is

a2=2F0/m

therefore the distance travel by the object from time t0 to 2t0 is calculated as

s2=(F0/m)*t0*t0+0.5(2F0/m)*(t0)^2

=(2F0/m)(t0)^2

Therefore total distance travel by the object is

S=s1+S2

=2.5(F0/m)(t0)^2

[(5F₀)/(2m)] t₀²

Further explanation

We deal with a case problem of uniformly accelerated motion and Newton's Second Law.

The formulas used are given by

[tex]\boxed{ \ F = ma \ } \ \boxed{ \ v = u + at \ } \ \boxed{ \ s = ut + \frac{1}{2}at^2 \ }[/tex]

  • F = force
  • m = mass
  • a = acceleration
  • u = initial velocity
  • v = final velocity
  • s = distance travelled
  • t = time taken

The first condition from t = 0 to t = t₀

A mass m is at rest on a horizontal frictionless surface at t = 0, thus the initial velocity [tex]\boxed{ \ u = 0 \ }.[/tex]

A constant force f₀ acts on it for a time t₀.

We call the acceleration in the first condition as a₁, i.e.,

[tex]\boxed{ \ a_1 = \frac{F_1}{m} \ } \rightarrow \boxed{ \ a_1 = \frac{F_0}{m} \ } \ (Equation-1)[/tex]

The final velocity at t = t₀ is given by

[tex]\boxed{ \ v_1 = 0 + a_1t_1 \ } \rightarrow \boxed{ \ v_1 = \Big( \frac{F_0}{m} \Big) t_0 \ } \ (Equation-2)[/tex]

The distance travelled from t = 0 to t = t₀ is given by

[tex]\boxed{ \ x_1 = (0)t + \frac{1}{2}a_1t_1^2 \ } \rightarrow \boxed{ \ x_1 = \frac{1}{2} \Big(\frac{F_0}{m} \Big)t_0^2 \ } \ (Equation-3)[/tex]

The second condition from t = t₀ to t = 2t₀

A constant force 2f₀ acts on it from t = t₀ to t = 2t₀.

We call the acceleration in the second condition as a₂.

[tex]\boxed{ \ a_2 = \frac{F_2}{m} \ } \rightarrow \boxed{ \ a_2 = \frac{2F_0}{m} \ } \ (Equation-4)[/tex]

The initial velocity of the second condition is precisely the final velocity of the first condition. We call back Equation-2.

[tex]\boxed{ \ u_2 = v_1 = \Big( \frac{F_0}{m} \Big) t_0 \ } \ (Equation-5)[/tex]

Time taken from t = t₀ to t = 2t₀ is [tex]\boxed{ \ t_2 = 2t_0 - t_0 \rightarrow t_2 = t_0 \ } \ Equation-6[/tex]

The distance travelled from t = 0 to t = t₀ is given by

[tex]\boxed{ \ x_2 = u_2t_2 + \frac{1}{2}a_2t_2^2 \ } \ (Equation-7)[/tex]

Substitute Equation-4, Equation-5, and Equation-6 into Equation-7.

[tex]\boxed{ \ x_2 = \Big( \frac{F_0}{m} \Big) t_0 \cdot t_0 + \frac{1}{2} \Big(\frac{2F_0}{m} \Big) t_0^2 \ }[/tex]

[tex]\boxed{ \ x_2 = \Big( \frac{F_0}{m} \Big) t_0^2 + \Big(\frac{F_0}{m} \Big) t_0^2 \ }[/tex]

[tex]\boxed{ \ x_2 = 2 \Big( \frac{F_0}{m} \Big) t_0^2 \ } \ (Equation-8)[/tex]

Determine the total distance

The total distance travelled from t = 0 to t = 2t₀ is obtained from the sum of Equation-3 and Equation-8.

[tex] \boxed{ \ x_{total} = x_1 + x_2 \ } [/tex]

[tex]\boxed{ \ x_{total} = \frac{1}{2} \Big(\frac{F_0}{m} \Big)t_0^2 + 2 \Big( \frac{F_0}{m} \Big) t_0^2 \ }[/tex]

[tex]\boxed{ \ x_{total} = \frac{1}{2} \Big(\frac{F_0}{m} \Big)t_0^2 + \frac{4}{2} \Big( \frac{F_0}{m} \Big) t_0^2 \ }[/tex]

Thus, the total distance travelled is [tex]\boxed{\boxed{ \ x_{total} = \frac{5}{2} \Big(\frac{F_0}{m} \Big) t_0^2 \ }}[/tex]

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Keywords: uniformly accelerated motion, Newton's second law, A mass, at rest on a horizontal frictionless, a constant force, for a time. suddenly the force doubles, determine the total distance travelled

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