Motion: Position, Velocity, Acceleration - Calculus 1

  1. A particle moves along a straight line. For a certain time interval, the particle's velocity is decreasing, but its speed is increasing. Which of the following statements must be true during that interval?
    Answer: The particle's velocity is negative and its acceleration is negative. 'Velocity is decreasing' means that the derivative of velocity, acceleration, is negative (a(t)<0a(t) < 0). 'Speed is increasing' means that velocity and acceleration have the same sign. Since we know acceleration is negative, velocity must also be negative (v(t)<0v(t) < 0). Therefore, the particle's velocity is negative and its acceleration is negative. This corresponds to moving in the negative direction and speeding up.
  2. A particle moves along the x-axis with velocity v(t)=3(t−1)(t−3)v(t) = 3(t-1)(t-3) for t≥0t \ge 0. For which of the following time intervals is the particle's displacement equal to the total distance it has traveled?
    Answer: [0,1][0, 1] A particle's displacement is equal to the total distance traveled over an interval if and only if the particle does not change direction on that interval. This means its velocity, v(t)v(t), must be either always non-negative or always non-positive throughout the interval. The velocity function is v(t)=3(t−1)(t−3)v(t) = 3(t-1)(t-3). The sign of v(t)v(t) changes at t=1t=1 and t=3t=3. v(t)≥0v(t) \ge 0 for t∈[0,1]∪[3,∞)t \in [0, 1] \cup [3, \infty). v(t)≤0v(t) \le 0 for t∈[1,3]t \in [1, 3]. Let's check the given intervals: - On [0,1][0, 1], v(t)≥0v(t) \ge 0, so the particle only moves in the positive direction. Displacement equals total distance. - On [1,3][1, 3], v(t)≤0v(t) \le 0, so the particle only moves in the negative direction. Displacement is negative while total distance is positive, so they are not equal. - On [0,2][0, 2], the particle moves in the positive direction for [0,1][0, 1] and in the negative direction for [1,2][1, 2]. Since it changes direction, displacement is not equal to total distance. - On [2,4][2, 4], the particle moves in the negative direction for [2,3][2, 3] and in the positive direction for [3,4][3, 4]. Since it changes direction, displacement is not equal to total distance.
  3. A particle moves along the x-axis with velocity v(t)=e−t(2t−t2)v(t) = e^{-t} (2t - t^2) for t>0t > 0. The particle's acceleration is zero at the exact moment its velocity reaches a local maximum. At what time tt does this occur?
    Answer: t=2+2t = 2 + \sqrt{2} The particle's acceleration is zero when its velocity reaches a local maximum. We need to find the time tt when a(t)=v′(t)=0a(t) = v'(t) = 0. Using the product rule for v(t)=e−t(2t−t2)v(t) = e^{-t} (2t - t^2): a(t)=(e−t)′(2t−t2)+e−t(2t−t2)′=−e−t(2t−t2)+e−t(2−2t)a(t) = (e^{-t})' (2t - t^2) + e^{-t} (2t - t^2)' = -e^{-t}(2t - t^2) + e^{-t}(2 - 2t). Set a(t)=0a(t) = 0: e−t[−(2t−t2)+(2−2t)]=0e^{-t} [-(2t - t^2) + (2 - 2t)] = 0. Since e−t>0e^{-t} > 0, we solve −2t+t2+2−2t=0  ⟹  t2−4t+2=0-2t + t^2 + 2 - 2t = 0 \implies t^2 - 4t + 2 = 0. Using the quadratic formula: t=4±16−4(1)(2)2=4±82=2±2t = \frac{4 \pm \sqrt{16 - 4(1)(2)}}{2} = \frac{4 \pm \sqrt{8}}{2} = 2 \pm \sqrt{2}. To determine which is a maximum, we can use the second derivative test for velocity, a′(t)a'(t), or analyze the sign of a(t)a(t). The parabola y=t2−4t+2y=t^2-4t+2 opens up, so it changes from + to - to + at its roots. The acceleration a(t)a(t) goes from positive to negative at the larger root, t=2+2t = 2 + \sqrt{2}, which indicates a local maximum for velocity.
  4. The position of a particle on the x-axis is s(t)=At2+Bt+Cs(t) = At^2 + Bt + C, where A, B, and C are non-zero constants. Which of the following statements about the particle's motion is true for all t>0t > 0?
    Answer: The particle's acceleration is always constant. Let's analyze the motion based on the position function s(t)=At2+Bt+Cs(t) = At^2 + Bt + C. The velocity is v(t)=s′(t)=2At+Bv(t) = s'(t) = 2At + B. The acceleration is a(t)=v′(t)=2Aa(t) = v'(t) = 2A. Since A is a non-zero constant, the acceleration 2A2A is also a non-zero constant. Thus, statement B is true. Statement A is false because v(t)v(t) is a linear function of tt, so speed ∣v(t)∣|v(t)| is not constant unless A=0A=0, which is ruled out. Statement C is false because v(t)=0v(t)=0 at t=−B/(2A)t = -B/(2A). This change of direction may or may not occur for t>0t>0, depending on the signs of A and B. Statement D is false because the particle is speeding up only when v(t)v(t) and a(t)a(t) have the same sign. It will slow down if their signs are different.
  5. A particle's velocity is given by v(t)=t2−8t+15v(t) = t^2 - 8t + 15. Which of the following statements correctly describes the motion of the particle at the exact moment its acceleration is zero?
    Answer: The particle has reached its minimum velocity. First, find the acceleration function a(t)=v′(t)a(t) = v'(t). a(t)=2t−8a(t) = 2t - 8. Set the acceleration to zero to find the time: 2t−8=0  ⟹  t=42t - 8 = 0 \implies t = 4. Now we analyze the particle's motion at t=4t=4. - Velocity at t=4t=4: v(4)=(4)2−8(4)+15=16−32+15=−1v(4) = (4)^2 - 8(4) + 15 = 16 - 32 + 15 = -1. Since v(4)≠0v(4) \neq 0, the particle is not at rest. - Change of direction: The particle changes direction when v(t)v(t) changes sign, which occurs when v(t)=0v(t)=0. t2−8t+15=(t−3)(t−5)=0t^2 - 8t + 15 = (t-3)(t-5)=0 at t=3t=3 and t=5t=5. The particle is not changing direction at t=4t=4. - The velocity function v(t)v(t) is a parabola that opens upward. Its minimum value occurs at its vertex. The time at which the vertex occurs is found by setting the derivative of v(t)v(t) to zero, which is v′(t)=a(t)=0v'(t) = a(t) = 0. We already found this occurs at t=4t=4. Therefore, at t=4t=4, the particle has reached its minimum velocity. - Speed is ∣v(t)∣|v(t)|. The speed at t=4t=4 is ∣−1∣=1|-1|=1. For large tt, v(t)v(t) grows infinitely large, so the speed is not at a maximum.
  6. A particle moves along a line such that its position is given by s(t)=t3−6t2+9t+1s(t) = t^3 - 6t^2 + 9t + 1 for t≥0t \ge 0. The particle is momentarily at rest at two different times. What is the magnitude of the difference in its acceleration at these two times?
    Answer: 1212 First, find the velocity function v(t)=s′(t)v(t) = s'(t). v(t)=3t2−12t+9v(t) = 3t^2 - 12t + 9. The particle is momentarily at rest when v(t)=0v(t) = 0. 3t2−12t+9=03t^2 - 12t + 9 = 0 t2−4t+3=0t^2 - 4t + 3 = 0 (t−1)(t−3)=0(t-1)(t-3) = 0 The particle is at rest at t=1t=1 and t=3t=3. Next, find the acceleration function a(t)=v′(t)a(t) = v'(t). a(t)=6t−12a(t) = 6t - 12. Now, calculate the acceleration at the two times when the particle is at rest: a(1)=6(1)−12=−6a(1) = 6(1) - 12 = -6. a(3)=6(3)−12=18−12=6a(3) = 6(3) - 12 = 18 - 12 = 6. The difference in the accelerations is a(3)−a(1)=6−(−6)=12a(3) - a(1) = 6 - (-6) = 12. The magnitude of this difference is ∣12∣=12|12| = 12.
  7. The position of a particle is s(t)=2sin⁡(t)−ts(t) = 2\sin(t) - t for 0≤t≤2π0 \le t \le 2\pi. For which of the following values of tt is the particle moving to the right and slowing down?
    Answer: t=π/6t = \pi/6 Moving right means v(t)>0v(t) > 0. Slowing down means v(t)v(t) and a(t)a(t) have opposite signs. So we need v(t)>0v(t) > 0 and a(t)<0a(t) < 0. First, find the functions: v(t)=s′(t)=2cos⁡(t)−1v(t) = s'(t) = 2\cos(t) - 1. a(t)=v′(t)=−2sin⁡(t)a(t) = v'(t) = -2\sin(t). Now we test the given points: A) At t=π/6t=\pi/6: v(π/6)=2cos⁡(π/6)−1=2(3/2)−1=3−1>0v(\pi/6) = 2\cos(\pi/6) - 1 = 2(\sqrt{3}/2) - 1 = \sqrt{3}-1 > 0. a(π/6)=−2sin⁡(π/6)=−2(1/2)=−1<0a(\pi/6) = -2\sin(\pi/6) = -2(1/2) = -1 < 0. Here, v>0v>0 and a<0a<0, so the particle is moving right and slowing down. B) At t=π/3t=\pi/3, v=0v=0. C) At t=2π/3t=2\pi/3, v<0v<0. D) At t=πt=\pi, v<0v<0.
  8. A particle moves on a line with velocity v(t)=t2−kt+4v(t) = t^2 - kt + 4, where kk is a constant. The particle is momentarily at rest at t=2t=2. What is the acceleration of the particle at this instant?
    Answer: 0 The particle is momentarily at rest when its velocity is zero. We are given this occurs at t=2t=2, so v(2)=0v(2)=0. Substitute t=2t=2 into the velocity function: v(2)=(2)2−k(2)+4=0v(2) = (2)^2 - k(2) + 4 = 0. This gives 4−2k+4=04 - 2k + 4 = 0, so 8−2k=08 - 2k = 0, which means k=4k=4. Now we know the full velocity function is v(t)=t2−4t+4v(t) = t^2 - 4t + 4. To find the acceleration, we differentiate the velocity: a(t)=v′(t)=2t−4a(t) = v'(t) = 2t - 4. Finally, we evaluate the acceleration at t=2t=2: a(2)=2(2)−4=0a(2) = 2(2) - 4 = 0.
  9. The velocity of a particle is v(t)=(t−1)(t−3)(t−5)v(t) = (t-1)(t-3)(t-5) for t≥0t \ge 0. Which statement best describes the particle's motion at t=2t=2?
    Answer: Moving right and slowing down. We need the signs of velocity v(t)v(t) and acceleration a(t)a(t) at t=2t=2. At t=2t=2, v(2)=(2−1)(2−3)(2−5)=(1)(−1)(−3)=3v(2) = (2-1)(2-3)(2-5) = (1)(-1)(-3) = 3. Since v(2)>0v(2) > 0, the particle is moving right. For acceleration, we first find the expression for v(t)=t3−9t2+23t−15v(t) = t^3 - 9t^2 + 23t - 15. Differentiating gives a(t)=v′(t)=3t2−18t+23a(t) = v'(t) = 3t^2 - 18t + 23. Now evaluate at t=2t=2: a(2)=3(22)−18(2)+23=12−36+23=−1a(2) = 3(2^2) - 18(2) + 23 = 12 - 36 + 23 = -1. Since v(2)>0v(2) > 0 and a(2)<0a(2) < 0, the signs are opposite, so the particle is slowing down. Thus, it is moving right and slowing down.
  10. The acceleration of a particle moving on a line is a(t)=12t2−18ta(t) = 12t^2 - 18t. At t=0t=0, the particle's velocity is v(0)=5v(0)=5 and its position is s(0)=2s(0)=2. At t=1t=1, what is the particle's velocity?
    Answer: 0 This question requires antidifferentiation. To find velocity v(t)v(t), we integrate acceleration a(t)a(t): v(t)=∫(12t2−18t)dt=4t3−9t2+Cv(t) = \int (12t^2 - 18t) dt = 4t^3 - 9t^2 + C. We use the initial condition v(0)=5v(0)=5 to find C: v(0)=4(0)3−9(0)2+C=5  ⟹  C=5v(0) = 4(0)^3 - 9(0)^2 + C = 5 \implies C=5. So the velocity function is v(t)=4t3−9t2+5v(t) = 4t^3 - 9t^2 + 5. Finally, we find the velocity at t=1t=1: v(1)=4(1)3−9(1)2+5=4−9+5=0v(1) = 4(1)^3 - 9(1)^2 + 5 = 4 - 9 + 5 = 0. The information about position s(0)s(0) is extra information not needed to solve for velocity.
  11. For a particle in rectilinear motion, its velocity v(t)v(t) is a differentiable function of time tt. For a specific time interval (a,b)(a, b), it is known that v(t)<0v(t) < 0 and the acceleration a(t)>0a(t) > 0. Which of the following statements must be true for the particle on the interval (a,b)(a, b)?
    Answer: The particle's speed is decreasing. The speed of the particle is given by ∣v(t)∣|v(t)|. A particle is speeding up if its velocity and acceleration have the same sign, and it is slowing down if they have opposite signs. - We are given that v(t)<0v(t) < 0, which means the particle is moving in the negative direction. Consequently, its position is decreasing, not increasing. - We are given that a(t)>0a(t) > 0. - Since v(t)v(t) and a(t)a(t) have opposite signs, the particle is slowing down. Its speed, ∣v(t)∣|v(t)|, is decreasing. - For the particle to change direction, its velocity v(t)v(t) must change sign. We are given that v(t)<0v(t) < 0 for the entire interval (a,b)(a, b), so it does not change direction.
  12. The position of a particle moving along a line is s(t)=t4−8t3+18t2s(t) = t^4 - 8t^3 + 18t^2. For what value of t>0t>0 is the particle's velocity at a minimum?
    Answer: t=3t=3 To find when velocity is at a minimum, we need to find the critical points of the velocity function by finding where its derivative (acceleration) is zero. First, find velocity: v(t)=s′(t)=4t3−24t2+36tv(t) = s'(t) = 4t^3 - 24t^2 + 36t. Now, find acceleration: a(t)=v′(t)=12t2−48t+36a(t) = v'(t) = 12t^2 - 48t + 36. Set a(t)=0a(t)=0: 12(t2−4t+3)=0  ⟹  12(t−1)(t−3)=012(t^2 - 4t + 3) = 0 \implies 12(t-1)(t-3)=0. The critical points for velocity are at t=1t=1 and t=3t=3. To determine which is a minimum, we use the second derivative test on velocity, which means finding the sign of a′(t)a'(t). a′(t)=24t−48a'(t) = 24t - 48. At t=1t=1, a′(1)=24−48=−24<0a'(1) = 24-48 = -24 < 0, indicating a local maximum for velocity. At t=3t=3, a′(3)=24(3)−48=72−48=24>0a'(3) = 24(3)-48 = 72-48 = 24 > 0, indicating a local minimum for velocity. Thus, velocity is at a minimum at t=3t=3.
  13. A particle moves on the x-axis with position given by s(t)=t3−6t2+5s(t) = t^3 - 6t^2 + 5 for t≥0t \ge 0. At which time t>0t>0 is the particle momentarily at rest after having moved in the negative direction?
    Answer: t=4t=4 First, find when the particle is at rest by setting the velocity v(t)=0v(t)=0. v(t)=s′(t)=3t2−12t=3t(t−4)v(t) = s'(t) = 3t^2 - 12t = 3t(t-4). The particle is at rest at t=0t=0 and t=4t=4. We are interested in t>0t>0, so we consider t=4t=4. Next, we must determine if the particle was moving in the negative direction just before t=4t=4. Moving in the negative direction means v(t)<0v(t) < 0. The sign of v(t)=3t(t−4)v(t) = 3t(t-4) is negative for tt between 0 and 4. So, on the interval (0,4)(0, 4), the particle is moving in the negative direction. Therefore, at t=4t=4, it comes to rest after having moved in the negative direction.
  14. The position of a particle is given by s(t)=8tt2+4s(t) = \frac{8t}{t^2+4} for t≥0t \ge 0. Which statement accurately describes the particle's motion at the instant it is farthest from the origin in the positive direction?
    Answer: Its velocity is zero and its acceleration is negative. The particle is farthest from the origin in the positive direction when its position s(t)s(t) is at a local maximum. This occurs when s′(t)=v(t)=0s'(t) = v(t) = 0 and s′′(t)=a(t)<0s''(t) = a(t) < 0 (by the Second Derivative Test). First, find the velocity: v(t)=s′(t)=8(t2+4)−8t(2t)(t2+4)2=32−8t2(t2+4)2v(t) = s'(t) = \frac{8(t^2+4) - 8t(2t)}{(t^2+4)^2} = \frac{32-8t^2}{(t^2+4)^2}. Setting v(t)=0v(t)=0 gives 32−8t2=032-8t^2=0, so t2=4t^2=4 and t=2t=2 (since t≥0t \ge 0). Now, find the acceleration at t=2t=2. a(t)=v′(t)=−16t(t2+4)2−(32−8t2)⋅2(t2+4)(2t)(t2+4)4a(t)=v'(t) = \frac{-16t(t^2+4)^2 - (32-8t^2) \cdot 2(t^2+4)(2t)}{(t^2+4)^4}. At t=2t=2, the numerator of v(t)v(t) is 0, so the second term of the numerator of a(t)a(t) is 0. Thus, a(2)=−16(2)(22+4)2(22+4)4=−32(8)2=−1/2a(2) = \frac{-16(2)(2^2+4)^2}{(2^2+4)^4} = \frac{-32}{(8)^2} = -1/2. Since v(2)=0v(2)=0 and a(2)<0a(2)<0, the particle is at a local maximum position.
  15. A particle's position is given by s(t)=2t3−21t2+60ts(t) = 2t^3 - 21t^2 + 60t for t≥0t \ge 0. What is the particle's velocity when its acceleration is zero?
    Answer: -13.5 This is a two-step problem. First, find the time when acceleration is zero. Then, find the velocity at that time. s(t)=2t3−21t2+60ts(t) = 2t^3 - 21t^2 + 60t. v(t)=s′(t)=6t2−42t+60v(t) = s'(t) = 6t^2 - 42t + 60. a(t)=v′(t)=12t−42a(t) = v'(t) = 12t - 42. Set a(t)=0a(t) = 0: 12t−42=0  ⟹  t=42/12=7/2=3.512t - 42 = 0 \implies t = 42/12 = 7/2 = 3.5. Now, substitute this time back into the velocity function: v(3.5)=6(3.5)2−42(3.5)+60=6(12.25)−147+60=73.5−147+60=−13.5v(3.5) = 6(3.5)^2 - 42(3.5) + 60 = 6(12.25) - 147 + 60 = 73.5 - 147 + 60 = -13.5.
  16. The position of a particle is given by s(t)=t3−12t2+36ts(t) = t^3 - 12t^2 + 36t for t≥0t \ge 0. At what time tt in the open interval (0,3)(0, 3) is the particle's instantaneous velocity equal to its average velocity on the closed interval [0,3][0, 3]?
    Answer: 4−74 - \sqrt{7} This question is an application of the Mean Value Theorem. First, calculate the average velocity on the interval [0,3][0, 3]. s(0)=03−12(0)2+36(0)=0s(0) = 0^3 - 12(0)^2 + 36(0) = 0. s(3)=33−12(3)2+36(3)=27−108+108=27s(3) = 3^3 - 12(3)^2 + 36(3) = 27 - 108 + 108 = 27. The average velocity is vavg=s(3)−s(0)3−0=273=9v_{avg} = \frac{s(3) - s(0)}{3 - 0} = \frac{27}{3} = 9. Next, find the instantaneous velocity function, v(t)=s′(t)v(t) = s'(t). v(t)=3t2−24t+36v(t) = 3t^2 - 24t + 36. Set the instantaneous velocity equal to the average velocity: 3t2−24t+36=93t^2 - 24t + 36 = 9 3t2−24t+27=03t^2 - 24t + 27 = 0 t2−8t+9=0t^2 - 8t + 9 = 0 Use the quadratic formula to solve for tt: t=−(−8)±(−8)2−4(1)(9)2(1)=8±64−362=8±282=8±272=4±7t = \frac{-(-8) \pm \sqrt{(-8)^2 - 4(1)(9)}}{2(1)} = \frac{8 \pm \sqrt{64 - 36}}{2} = \frac{8 \pm \sqrt{28}}{2} = \frac{8 \pm 2\sqrt{7}}{2} = 4 \pm \sqrt{7}. The two possible times are t=4−7t = 4 - \sqrt{7} and t=4+7t = 4 + \sqrt{7}. We must determine which of these lies in the interval (0,3)(0, 3). Since 2<7<32 < \sqrt{7} < 3, we have: t1=4−7≈4−2.65=1.35t_1 = 4 - \sqrt{7} \approx 4 - 2.65 = 1.35. This is in (0,3)(0, 3). t2=4+7≈4+2.65=6.65t_2 = 4 + \sqrt{7} \approx 4 + 2.65 = 6.65. This is not in (0,3)(0, 3). Therefore, the correct time is t=4−7t = 4 - \sqrt{7}.
  17. A particle moves along a line with acceleration a(t)=4t−10a(t) = 4t - 10. At time t=0t=0, its velocity is v(0)=8v(0) = 8. For t≥0t \ge 0, what is the minimum speed of the particle?
    Answer: 00 First, we need to find the velocity function v(t)v(t) by integrating the acceleration function a(t)a(t). v(t)=∫a(t) dt=∫(4t−10) dt=2t2−10t+Cv(t) = \int a(t) \,dt = \int (4t - 10) \,dt = 2t^2 - 10t + C. We use the initial condition v(0)=8v(0)=8 to find the constant CC. v(0)=2(0)2−10(0)+C=8  ⟹  C=8v(0) = 2(0)^2 - 10(0) + C = 8 \implies C = 8. So, the velocity function is v(t)=2t2−10t+8v(t) = 2t^2 - 10t + 8. Speed is the absolute value of velocity, ∣v(t)∣|v(t)|. To find the minimum speed, we must find the minimum value of ∣2t2−10t+8∣|2t^2 - 10t + 8|. The minimum value of an absolute value function can be 0 if the function itself can be 0. Let's check if the particle ever stops, i.e., if v(t)=0v(t)=0. 2t2−10t+8=02t^2 - 10t + 8 = 0 2(t2−5t+4)=02(t^2 - 5t + 4) = 0 2(t−1)(t−4)=02(t-1)(t-4) = 0 The velocity is zero at t=1t=1 and t=4t=4. When the velocity is zero, the speed is also zero. Since speed cannot be negative, the minimum possible speed is 0. This minimum is achieved at t=1t=1 and t=4t=4.
  18. The position of a particle on the x-axis is given by s(t)=t3−6t2+9t+1s(t) = t^3 - 6t^2 + 9t + 1 for t≥0t \ge 0. What is the total distance traveled by the particle from t=0t=0 to t=2t=2?
    Answer: 6 Total distance requires accounting for any changes in direction. First, find the velocity: v(t)=s′(t)=3t2−12t+9=3(t−1)(t−3)v(t) = s'(t) = 3t^2 - 12t + 9 = 3(t-1)(t-3). The particle changes direction when v(t)v(t) changes sign, which occurs at t=1t=1 and t=3t=3. Within the interval [0,2][0, 2], there is a change of direction at t=1t=1. We must calculate the distance traveled on [0,1][0, 1] and [1,2][1, 2] separately. Positions are: s(0)=1s(0) = 1, s(1)=1−6+9+1=5s(1) = 1-6+9+1=5, and s(2)=8−24+18+1=3s(2) = 8-24+18+1=3. The distance traveled from t=0t=0 to t=1t=1 is ∣s(1)−s(0)∣=∣5−1∣=4|s(1)-s(0)| = |5-1| = 4. The distance traveled from t=1t=1 to t=2t=2 is ∣s(2)−s(1)∣=∣3−5∣=2|s(2)-s(1)| = |3-5| = 2. The total distance is 4+2=64+2=6.
  19. A particle moves along a line with acceleration a(t)=2ta(t) = 2t. Its velocity at t=3t=3 is v(3)=5v(3)=5. What is its average velocity over the interval [0,3][0, 3]?
    Answer: -1 First, find the velocity function by integrating acceleration: v(t)=∫2tdt=t2+Cv(t) = \int 2t dt = t^2 + C. Use the condition v(3)=5v(3)=5 to find C: 32+C=5  ⟹  9+C=5  ⟹  C=−43^2+C=5 \implies 9+C=5 \implies C=-4. So, v(t)=t2−4v(t) = t^2-4. Average velocity over [0,3][0, 3] is given by s(3)−s(0)3−0\frac{s(3)-s(0)}{3-0}, which requires finding the position function s(t)s(t). s(t)=∫(t2−4)dt=13t3−4t+Ds(t) = \int (t^2-4) dt = \frac{1}{3}t^3 - 4t + D. The displacement is s(3)−s(0)=(13(3)3−4(3)+D)−(13(0)3−4(0)+D)=(9−12)−0=−3s(3)-s(0) = (\frac{1}{3}(3)^3 - 4(3) + D) - (\frac{1}{3}(0)^3 - 4(0) + D) = (9-12) - 0 = -3. The average velocity is −33−0=−1\frac{-3}{3-0} = -1.
  20. The position of a particle moving on the x-axis is given by s(t)=et(t2−3)s(t) = e^t(t^2 - 3) for t≥0t \ge 0. For what open interval of time tt is the particle moving toward the origin?
    Answer: (1,3)(1, \sqrt{3}) A particle is moving toward the origin when its position and velocity have opposite signs. This means we need to find where (s(t)>0s(t) > 0 and v(t)<0v(t) < 0) or (s(t)<0s(t) < 0 and v(t)>0v(t) > 0). 1. Find the sign of position s(t)=et(t2−3)s(t) = e^t(t^2 - 3). Since ete^t is always positive, the sign of s(t)s(t) is determined by the sign of t2−3t^2 - 3. For t≥0t \ge 0, s(t)<0s(t) < 0 when t2<3t^2 < 3, i.e., on [0,3)[0, \sqrt{3}). s(t)>0s(t) > 0 when t2>3t^2 > 3, i.e., on (3,∞)(\sqrt{3}, \infty). 2. Find the velocity v(t)=s′(t)v(t) = s'(t) using the product rule: v(t)=et(t2−3)+et(2t)=et(t2+2t−3)=et(t+3)(t−1)v(t) = e^t(t^2 - 3) + e^t(2t) = e^t(t^2 + 2t - 3) = e^t(t+3)(t-1). Since ete^t and (t+3)(t+3) are positive for t≥0t \ge 0, the sign of v(t)v(t) is determined by the sign of (t−1)(t-1). Thus, v(t)<0v(t) < 0 on [0,1)[0, 1) and v(t)>0v(t) > 0 on (1,∞)(1, \infty). 3. Combine the results. We need s(t)s(t) and v(t)v(t) to have opposite signs. - On [0,1)[0, 1): s(t)<0s(t) < 0 and v(t)<0v(t) < 0. Same signs. Moving away from the origin. - On (1,3)(1, \sqrt{3}): s(t)<0s(t) < 0 and v(t)>0v(t) > 0. Opposite signs. Moving toward the origin. - On (3,∞)(\sqrt{3}, \infty): s(t)>0s(t) > 0 and v(t)>0v(t) > 0. Same signs. Moving away from the origin. The particle is moving toward the origin on the interval (1,3)(1, \sqrt{3}).

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