# Section 3 2 Motion with Constant Acceleration In

- Slides: 35

Section 3. 2 Motion with Constant Acceleration In this section you will: ● Interpret position-time graphs for motion with constant acceleration. ● Determine mathematical relationships among position, velocity, acceleration, and time. ● Apply graphical and mathematical relationships to solve problems related to constant acceleration.

Section 3. 2 Motion with Constant Acceleration Velocity with Average Acceleration If an object’s average acceleration during a time interval is known, then it can be used to determine how much the velocity changed during that time. The definition of average acceleration: can be rewritten as follows:

Section 3. 2 Motion with Constant Acceleration Velocity with Average Acceleration The equation for final velocity with average acceleration can be written as follows: The final velocity is equal to the initial velocity plus the product of the average acceleration and time interval.

Section 3. 2 Motion with Constant Acceleration Velocity with Average Acceleration In cases in which the acceleration is constant, the average acceleration, ā, is the same as the instantaneous acceleration, a. The equation for final velocity can be rewritten to find the time at which an object with constant acceleration has a given velocity. It also can be used to calculate the initial velocity of an object when both the velocity and the time at which it occurred are given.

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration The position data at different time intervals for a car with constant acceleration are shown in the table. The data from the table are graphed as shown on the next slide.

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration The graph shows that the car’s motion is not uniform: the displacements for equal time intervals on the graph get larger and larger. The slope of a position-time graph of a car moving with a constant acceleration gets steeper as time goes on.

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration The slopes from the position time graph can be used to create a velocity-time graph as shown on the right. Note that the slopes shown in the position-time graph are the same as the velocities graphed in the velocity-time graph.

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration A unique position-time graph cannot be created using a velocity-time graph because it does not contain any information about the object’s position. However, the velocity-time graph does contain information about the object’s displacement. Recall that for an object moving at a constant velocity,

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration On the graph shown on the right, v is the height of the plotted line above the t-axis, while Δt is the width of the shaded rectangle. The area of the rectangle, then, is vΔt, or Δd. Thus, the area under the v-t graph is equal to the object’s displacement.

Section 3. 2 Motion with Constant Acceleration Position with Constant Acceleration The area under the v-t graph is equal to the object’s displacement.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph The v-t graph shows the motion of an airplane. Find the displacement of the airplane at Δt = 1. 0 s and at Δt = 2. 0 s.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Step 1: Analyze and Sketch the Problem

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph The displacement is the area under the v-t graph.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph The time intervals begin at t = 0. 0.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v -t Graph Identify the known and unknown variables. Known: Unknown: v = +75 m/s Δd = ? Δt = 1. 0 s Δt = 2. 0 s

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Step 2: Solve for the Unknown

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Solve for displacement during Δt = 1. 0 s.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Substitute v = +75 m/s, Δt = 1. 0 s

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Solve for displacement during Δt = 2. 0 s.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Substitute v = +75 m/s, Δt = 2. 0 s

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Step 3: Evaluate the Answer

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph Are the units correct? Displacement is measured in meters. Do the signs make sense? The positive sign agrees with the graph. Is the magnitude realistic? Moving a distance of about one football field in 2 s is reasonable for an airplane.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph The steps covered were: Step 1: Analyze and Sketch the Problem The displacement is the area under the v-t graph. The time intervals begin at t = 0. 0. Step 2 Solve for the Unknown Solve for displacement during Δt = 1. 0 s. Solve for displacement during Δt = 2. 0 s.

Section 3. 2 Motion with Constant Acceleration Finding the Displacement from a v-t Graph The steps covered were: Step 3: Evaluate the Answer

Section 3. 2 Motion with Constant Acceleration An Alternative Expression Often, it is useful to relate position, velocity, and constant acceleration without including time. The three equations for motion with constant acceleration are summarized in the table.

Section 3. 2 Motion with Constant Acceleration An Alternative Expression Rearrange the equation vf = vi + ātf, to solve for time:

Section 3. 2 Motion with Constant Acceleration An Alternative Expression This equation can be solved for the velocity, vf, at any time, tf. The square of the final velocity equals the sum of the square of the initial velocity and twice the product of the acceleration and the displacement since the initial time.

Section 3. 2 Section Check Question 1 A position-time graph of a bike moving with constant acceleration is shown below. Which statement is correct regarding the displacement of the bike?

Section 3. 2 Section Check Question 1 A. The displacement in equal time intervals is constant. B. The displacement in equal time intervals progressively increases. C. The displacement in equal time intervals progressively decreases. D. The displacement in equal time intervals first increases, then after reaching a particular point, it decreases.

Section 3. 2 Section Check Answer 1 Reason: You will see that the slope gets steeper as time progresses, which means that the displacement in equal time intervals progressively gets larger and larger.

Section 3. 2 Section Check Question 2 A car is moving with an initial velocity of vi m/s. After reaching a highway, it moves with a constant acceleration of a m/s 2, what will be the velocity (vf) of the car after traveling for t seconds? A. vf = vi + at B. vf = vi + 2 at C. vf 2 = vi 2 + 2 at D. vf = vi – at

Section 3. 2 Section Check Answer 2 Reason: Since a = Δv/Δt vf - vi = a (tf - ti) Also since the car is starting from rest, ti = 0 Therefore vf = vi + at (where t is the total time)

Section 3. 2 Section Check Question 3 From the graph as shown on the right, if a car slowing down with a constant acceleration from initial velocity vi to the final velocity vf, calculate the total distance (Δd) traveled by the car. A. C. B. D.

Section 3. 2 Section Check Answer 3 Reason: Acceleration is the area under the graph. Solving for Δd, we get

Section 3. 2 Section Check Answer 3 Reason: Now since (vf – vi) = aΔt (vi – vf) = –aΔt Substituting in the above equation, we get Δdtriangle = –a(Δt)2 Also Δdrectangle = vf(Δt) Adding the above two equations, we can write Δd = vf(Δt) – a(Δt)2

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