Non-uniform acceleration *

Size: px

Start display at page:

Download "Non-uniform acceleration *"

Barnard Washington
5 years ago
Views:

1 OpenStax-CNX module: m Non-uniform acceleration * Sunil Kumar Singh This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License 2.0 Non-uniform acceleration constitutes the most general description of motion. It refers to variation in the rate of change in velocity. Simply put, it means that acceleration changes during motion. This variation can be expressed either in terms of position (x) or time (t). We understand that if we can describe non-uniform acceleration in one dimension, we can easily extend the analysis to two or three dimensions using composition of motions in component directions. For this reason, we shall conne ourselves to the consideration of nonuniform i.e. variable acceleration in one dimension. In this module, we shall describe non-uniform acceleration using expressions of velocity or acceleration in terms of either of time, t, or position, x. We shall also consider description of non-uniform acceleration by expressing acceleration in terms of velocity. As a matter of fact, there can be various possibilities. Besides, non-uniform acceleration may involve interpretation acceleration - time or velocity - time graphs. Accordingly, analysis of non-uniform acceleration motion is carried out in two ways : Using calculus Using graphs Analysis using calculus is generic and accurate, but is limited to the availability of expression of velocity and acceleration. It is not always possible to obtain an expression of motional attributes in terms of x or t. On the other hand, graphical method lacks accuracy, but this method can be used with precision if the graphs are composed of regular shapes. Using calculus involves dierentiation and integration. The integration allows us to evaluate expression of acceleration for velocity and evaluate expression of velocity for displacement. Similarly, dierentiation allows us to evaluate expression of position for velocity and evaluate expression of velocity for acceleration. We have already worked with expression of position in time. We shall work here with other expressions. Clearly, we need to know a bit about dierentiation and integration before we proceed to analyze non-uniform motion. 1 Important calculus results Integration is anti-dierentiation i.e. an inverse process. We can compare dierentiation and integration of basic algebraic, trigonometric, exponential and logarithmic functions to understand the inverse relation between processes. In the next section, we list few important dierentiation and integration results for reference. 1.1 Dierentiation x xn = nx n 1 ; x (ax + b)n = na(ax + b) n 1 * Version 1.2: Sep 28, :51 am

2 OpenStax-CNX module: m sinax = acosax; x x x ex = e x ; cosax = asinax x log ex = 1 x 1.2 Integration x n x = xn+1 n + 1 ; (ax + b) n x = sinaxx = cosax ; a e x x = e x ; (ax + b)n+1 a (n + 1) cosaxx = sinax a x x = log ex 2 Velocity and acceleration is expressed in terms of time t Let the expression of acceleration in x is given as function a(t). Now, acceleration is related to velocity as : a (t) = v t We obtain expression for velocity by rearranging and integrating : v = a (t) t v = a (t) t This relation yields an expression of velocity in "t" after using initial conditions of motion. We obtain expression for position/ displacement by using dening equation, rearranging and integrating : v (t) = dx dt x = v (t) t x = v (t) t This relation yields an expression of position in "t" after using initial conditions of motion. Example 1 Problem : The acceleration of a particle along x-axis varies with time as : a = t 1 Velocity and position both are zero at t= 0. Find displacement of the particle in the interval from t=1 to t = 3 s. Consider all measurements in SI unit. Solution : Using integration result obtained earlier for expression of acceleration : v = v 2 v 1 = a (t) t

3 OpenStax-CNX module: m Here, v 1 = 0. Let v 2 = v, then : v = t 0 a (t) t = t 0 (t 1) t Note that we have integrated RHS between time 0 ans t seconds in order to get an expression of velocity in t. v = t2 2 t Using integration result obtained earlier for expression of velocity : ( ) t 2 x = v (t) t = 2 t dt Integrating between t=1 and t=3, we have : x = 3 1 ( ) [ t 2 t 3 2 t t = 6 t2 2 ] 3 1 = = 5 4 = 1m Example 2 Problem : If the velocity of particle moving along a straight line is proportional to 3 th 4 power of time, then how do its displacement and acceleration vary with time? Solution : Here, we need to nd a higher order attribute (acceleration) and a lower order attribute displacement. We can nd high order attribute by dierentiation, whereas we can nd lower order attribute by integration. Let, v t 3 4 v = kt 3 4 where k is a constant. The acceleration of the particle is : Hence, a = v ( t ) t = 3kt = 3kt v t 1 4 For lower order attribute displacement, we integrate the function : x = v t x = v t = kt 3 4 t = 4kt x t 7 4

4 OpenStax-CNX module: m Velocity and acceleration is expressed in terms of time x Let the expression of acceleration in x given as function a(x). Now, the dening equation of instantaneous acceleration is: a (x) = v t In order to incorporate dierentiation with position, x, we rearrange the equation as : a (x) = v x X x t = vv x We obtain expression for velocity by rearranging and integrating : vdv = a (x) dx This relation yields an expression of velocity in x. We obtain expression for position/ displacement by using dening equation, rearranging and integrating : This relation yields an expression of position in t. v (x) = x t t = x v (x) x t = v (x) Example 3 Problem : The acceleration of a particle along x-axis varies with position as : a = 9x Velocity is zero at t = 0 and x=2m. Find speed at x=4. Consider all measurements in SI unit. Solution : Using integration, vv = a (x) x v 0 [ v 2 2 vv = ] v 0 x 9xx 2 [ x 2 = 9 2 v2 2 = 9x ] x v 2 = 9x 2 36 = 9 ( x 2 4 ) 2 v = ±3 (x 2 4) We neglect negative sign as particle is moving in x-direction with positive acceleration. At x =4 m,

5 OpenStax-CNX module: m v = 3 (4 2 4) = 3 12 = 6 3 m/s 4 Acceleration in terms of velocity Let acceleration is expressed as function of velocity as : a = a (v) 4.1 Obtaining expression of velocity in time, t The acceleration is dened as : Arranging terms with same variable on one side of the equation, we have : Integrating, we have : t = v a (v) t = v a (v) Evaluation of this relation results an expression of velocity in t. Clearly, we can proceed as before to obtain expression of position in t. 4.2 Obtaining expression of velocity in time, x In order to incorporate dierentiation with position, x, we rearrange the dening equation of acceleration as : a (v) = v x X x t = vv x Arranging terms with same variable on one side of the equation, we have : Integrating, we have : x = vv a (v) x = vv a (v) Evaluation of this relation results an expression of velocity in x. Clearly, we can proceed as before to obtain expression of position in t. Example 4 Problem : The motion of a body in one dimension is given by the equation dv(t)/dt = v (t), where v(t) is the velocity in m/s and t in seconds. If the body was at rest at t = 0, then nd the expression of velocity. Solution : Here, acceleration is given as a function in velocity as independent variable. We are required to nd expression of velocity in time. Using integration result obtained earlier for expression of time : t = v a (v)

6 OpenStax-CNX module: m Substituting expression of acceleration and integrating between t=0 and t=t, we have : t = t = v ( t ) 6 3v ( t ) t = ln [ { 6 3v ( t ) 6 ] 3 6 3v ( t ) = 6e 3t 3v ( t ) = 6 ( 1 e ) 3t v ( t ) = 2 ( 1 e ) 3t 5 Graphical method We analyze graphs of motion in parts keeping in mind regular geometric shapes involved in the graphical representation. Here, we shall work with two examples. One depicts variation of velocity with respect to time. Other depicts variation of acceleration with respect to time. 5.1 Velocity.vs. time Example 5 Problem : below : A particle moving in a straight line is subjected to accelerations as given in the gure Acceleration time plot Figure 1: Acceleration time plot

7 OpenStax-CNX module: m If v = 0 and t = 0, then draw velocity time plot for the same time interval. Solution : In the time interval between t = 0 and t = 2 s, acceleration is constant and is equal to 2 m / s 2. Hence, applying equation of motion for nal velocity, we have : But, u = 0 and a = 2 m / s 2. v = u + at v = 2t The velocity at the end of 2 seconds is 4 m/s. Since acceleration is constant, the velocity time plot for the interval is a straight line. On the other hand, the acceleration is zero in the time interval between t = 2 and t = 4 s. Hence, velocity remains constant in this time interval. For time interval t = 4 and 6 s, acceleration is - 4 m / s 2. From the plot it is clear that the velocity at t = 4 s is equal to the velocity at t = 2 s, which is given by : u = 2 x 2 = 4 m / s Velocity time plot Figure 2: Corresponding velocity time plot. Putting this value as initial velocity in the equation of velocity, we have : v = 4 4t

8 OpenStax-CNX module: m We should, however, be careful in drawing velocity plot for t = 4 s to t = 6 s. We should relaize that the equation above is valid in the time interval considered. The time t = 4 s from the beginning corresponds to t = 0 s and t = 6 s corresponds to t = 2 s for this equation. Velocity at t = 5 s is obtained by putting t = 1 s in the equation, v = 4 4 x 1 = 0 Velocity at t = 6 s is obtained by putting t = 2 s in the equation, v = 4 4 x 2 = 4 m / s 5.2 Acceleration.vs. time Example 6 Problem : A particle starting from rest and undergoes a rectilinear motion with acceleration a. The variation of a with time t is shown in the gure. Find the maximum velocity attained by the particle during the motion. Acceleration time plot Figure 3: The area under plot gives change in velocity. Solution : We see here that the particle begins from rest and is continuously accelerated in one direction (acceleration is always positive through out the motion) at a diminishing rate. Note that though acceleration is decreasing, but remains positive for the motion. It means that the particle attains maximum velocity at the end of motion i.e. at t = 12 s. The area under the plot on acceleration time graph gives change in velocity. Since the plot start at t = 0 i.e. the beginning of the motion, the areas under the plot gives the velocity at the end of motion,

9 OpenStax-CNX module: m v = v 2 v 1 = v 0 = v = 1 2 x 8 x 12 = 48 m / s v max = 48 m / s 6 Exercises First identify : what is given and what is required. Establish relative order between given and required attribute. Use dierentiation method to get a higher order attribute in the following order : displacement (position vector) velocity acceleration. Use integration method to get a lower order attribute in the following order : acceleration velocity displacement (position vector). Since we are considering accelerated motion in one dimension, graphical representation of motion is valid. The interpretation of plot in terms of slope of the curve gives higher order attribute, whereas interpretation of plot in terms of area under the plot gives lower order attribute. Exercise 1 (Solution on p. 11.) A particle of mass m moves on the x-axis. It starts from rest t = 0 from the point x = 0, and comes to rest at t = 1 at the point x = 1. No other information is available about its motion at intermediate time (0 < t < 1). Prove that magnitude of instantaneous acceleration during the motion can not be less than 4 m / s 2. Exercise 2 (Solution on p. 12.) A particle accelerates at constant rate a from rest at and then decelerates at constant rate b to come to rest. If the total time elapsed is t during this motion, then nd (i) maximum velocity achieved and (ii) total displacement during the motion. Velocity time plot Figure 4: acceleration. Area under velocity time plot gives displacement, whereas slope of the plot gives the

10 OpenStax-CNX module: m Exercise 3 (Solution on p. 13.) The velocity time plot of the motion of a particle along x - axis is as shown in the gure. If x = 0 at t= 0, then (i) analyze acceleration of particle during the motion (ii) draw corresponding displacement time plot (showing nature of the plot) and (iii) nd total displacement. Velocity time plot Figure 5: Slope of the plot gives acceleration; area under plot gives displacement. Exercise 4 (Solution on p. 14.) The motion of a body in one dimension is given by the equation dv(t)/dt = v (t), where v(t) is the velocity in m/s and t in seconds. If the body was at rest at t = 0, then nd the terminal speed. Exercise 5 (Solution on p. 15.) The motion of a body in one dimension is given by the equation dv(t)/dt = v (t), where v(t) is the velocity in m/s and t in seconds. If the body was at rest at t = 0, then nd the magnitude of the initial acceleration and also nd the velocity, when the acceleration is half the initial value.

11 OpenStax-CNX module: m Solutions to Exercises in this Module Solution to Exercise (p. 9) In between the starting and end point, the particle may undergo any combination of acceleration and deceleration. According to question, we are required to know the minimum value of acceleration for any combination possible. Let us check the magnitude of acceleration for the simplest combination and then we evaluate other complex possible scenarios. Now, the simplest scenario would be that the particle rst accelerates and then decelerates for equal time and at the same rate to complete the motion. Velocity time plot Figure 6: Velocity time plot In order to assess the acceleration for a linear motion, we would make use of the fact that area under v-t plot gives the displacement (= 1 m). Hence, OAB = 1 2 x vt = 1 2 x v x 1 = 1 m v max = 2 m / s Thus, the maximum velocity during motion under this condition is 2 m/s. acceleration for this motion is equal to the slope of the line, On the other hand, the a = tanθ = = 4 m / s2 Now let us complicate the situation, in which particle accelerates for shorter period and decelerates gently for a longer period (see gure below). This situation would result velocity being equal to 2 m/s and acceleration greater than 4 m / s 2. It is so because time period is xed (1 s) and hence base of the triangle is xed. Also as displacement in given time is 1 m. It means that area under the triangle is also xed (1 m). As area is half of the product of base and height, it follows that the height of the triangle should remain same i.e 2 m/s. For this reason the graphical representations of possible variation of acceleration and deceleration may look like as shown in the gure here.

12 OpenStax-CNX module: m Velocity time plot Figure 7: acceleration. Area under velocity time plot gives displacement, whereas slope of the plot gives the Clearly, the slope of OA' is greater than 4 m / s 2. We may argue that why to have a single combination of acceleration and deceleration? What if the particle undergoes two cycles of acceleration and deceleration? It is obvious that such consideration will again lead to similar analysis for symmetric and non-symmetric acceleration, which would be bounded by the value of time and area of the triangle. Thus we conclude that the minimum value of acceleration is 4 m / s 2. Solution to Exercise (p. 9) The particle initially accelerates at a constant rate. It means that its velocity increases with time. The particle, therefore, gains maximum velocity say, v max, before it begins to decelerate. Let t 1 and t 2 be the time intervals, for which particle is in acceleration and deceleration respectively. Then, t = t 1 + t 2 From the triangle OAC, the magnitude of acceleration is equal to the slope of straight line OA. Hence, a = vmax t 1 Similarly from the triangle CAB, the magnitude of acceleration is equal to the slope of straight line AB. Hence, Substituting values of time, we have : t = vmax a b = vmax t 2 + vmax b = v max ( a + b ab ) v max = abt ( a + b )

13 OpenStax-CNX module: m In order to nd the displacement, we shall use the fact that area under velocity time plot is equal to displacement. Hence, x = 1 2 Putting the value of maximum velocity, we have : x v maxt x = abt 2 2 ( a + b ) Solution to Exercise (p. 10) Graphically, slope of the plot yields acceleration and area under the plot yields displacement. Since the plot involves regular geometric shapes, we shall nd areas of these geometric shapes individually and then add them up to get various points for displacement time plot. The displacement between times 0 and 1 s is : x = 1 2 x 1 x 10 = 5m The velocity between 0 and 1 s is increasing at constant rate. The acceleration is constant and its magnitude is equal to the slope, which is 101 = 10 m / s 2. Since acceleration is in the direction of motion, the particle is accelerated. The resulting displacement time curve is a parabola with an increasing slope. The displacement between times 1 and 2 s is : x = 1 x 10 = 10m The velocity between 1 and 2 s is constant and as such acceleration is zero. The resulting displacement time curve for this time interval is a straight line having slope equal to that of the magnitude of velocity. The displacement at the end of 2 s is = 15 m Now, the displacement between times 2 and 4 s is : x = 1 2 x ( ) x 1 = 25m

14 OpenStax-CNX module: m Displacement time plot Figure 8: Corresponding displacement time plot of the given velocity- - time plot. The velocity between 2 and 4 s is increasing at constant rate. The acceleration, therefore, is constant and its magnitude is equal to the slope of the plot, 202 = 10 m / s 2. Since acceleration is in the direction of motion, the particle is accelerated and the resulting displacement time curve is a parabola with increasing slope. The displacement at the end of 4 s is = 40 m Now, the displacement between times 4 and 5 s is : x = 1 2 x 30 x 1 = 15m The velocity between 2 and 4 s is decreasing at constant rate, but always remains positive. As such, the acceleration is constant, but negative and its magnitude is equal to the slope, which is 301 = 30 m / s 2. Since acceleration is in the opposite direction of motion, the particle is decelerated. The resulting displacement time curve is an inverted parabola with decreasing slope. The nal displacement at the end of 5 s is = 55 m Characteristics of motion : One dimensional, Unidirectional, variable acceleration in one dimension (magnitude)

15 OpenStax-CNX module: m Solution to Exercise (p. 10) In order to answer this question, we need to know the meaning of terminal speed. The terminal speed is the speed when the body begins to move with constant speed. Now, the rst time derivate of velocity gives the acceleration of the body : For terminal motion, a = 0. Hence, v ( t ) t = a = 6 3v ( t ) a = 6 3v ( t ) = 0 v ( t ) = 6 3 = 2 m / s Solution to Exercise (p. 10) We have to nd the acceleration at t = 0 from the equation given as : v ( t ) t = a = 6 3v ( t ) Generally, we would have been required to know the velocity function so that we can evaluate the function for time t = 0. In this instant case, though the function of velocity is not known, but we know the value of velocity at time t = 0. Thus, we can know acceleration at t =0 by just substituting the value for velocity function at that time instant as : a = 6 3v ( t ) = 6 3 x 0 = 6 m / s 2 Now when the acceleration is half the initial acceleration, a = a 2 = 6 2 = 3 m / s2 Hence, 6 3v ( t ) = 3 v ( t ) = 3 3 = 1 m / s

Domain and range of exponential and logarithmic function *

OpenStax-CNX module: m15461 1 Domain and range of exponential and logarithmic function * Sunil Kumar Singh This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License