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title: "Distance vs Displacement: Integrating |v(t)| Correctly" slug: distance-vs-displacement-integrating-vt-correctly tags: ["dynamics", "kinematics", "distance", "displacement", "velocity"] generated_at: 2026-04-23T16:50:46.190944+00:00 generator_model: gpt-4o-mini-2024-07-18 source_notes: ["20260422013117-acceleration", "20260422013117-velocity-function", "20260422013117-position-function", "20260422013117-acceleration-function", "20260422013117-average-velocity"] ai_disclosure: "Generated from personal class notes with AI assistance. Every factual claim cites a note."

Distance vs Displacement: Integrating |v(t)| Correctly

Abstract

In the study of dynamics, distinguishing between distance and displacement is crucial for accurately interpreting motion. This article explores the integration of the absolute value of the velocity function, v(t)|v(t)|, to compute distance traveled, contrasting it with the calculation of displacement through direct integration of the velocity function. By examining the mathematical foundations and providing illustrative examples, we clarify the differences between these two concepts and their implications in kinematic analysis.

Background

In kinematics, distance and displacement are fundamental concepts that describe motion. Distance refers to the total length of the path traveled by an object, regardless of direction, while displacement is a vector quantity that measures the shortest straight-line distance from the initial to the final position. Understanding how to calculate both quantities is essential for analyzing motion accurately.

The velocity function, which represents the rate of change of position with respect to time, is given by:

v(t)=dsdtv(t) = \frac{ds}{dt}

where vv is the velocity in meters per second and tt is the time in seconds [velocity-function]. The relationship between velocity, distance, and displacement becomes particularly important when the motion involves changes in direction. This distinction is not merely academic; it has practical implications in physics, engineering, and applied mathematics where precise characterization of motion is required.

Key Results

To compute displacement, we integrate the velocity function over a specified time interval. For a particle with a velocity function defined as:

v(t)=2t6v(t) = 2t - 6

the displacement ss from time t0t_0 to t1t_1 can be calculated using:

s=t0t1v(t)dts = \int_{t_0}^{t_1} v(t) \, dt

This integral yields the net change in position, which can be positive or negative depending on the direction of motion [position-function]. When velocity is negative, the object moves in the negative direction, and this is reflected in the displacement calculation.

In contrast, to find the total distance traveled, we must consider the absolute value of the velocity function:

d=t0t1v(t)dtd = \int_{t_0}^{t_1} |v(t)| \, dt

This approach accounts for any changes in direction, ensuring that the distance is always a non-negative quantity. The absolute value function removes the sign information, treating all motion as contributing positively to the total path length. This is a critical distinction because distance accumulates regardless of direction, whereas displacement can cancel out when an object reverses course.

Worked Examples

Consider a particle whose position function is given by:

s(t)=10t2+20s(t) = 10t^2 + 20

From this, we can derive the velocity function:

v(t)=dsdt=20tv(t) = \frac{ds}{dt} = 20t

Now, if we analyze the motion over the interval from t=0t = 0 to t=3t = 3:

Displacement Calculation

First, we compute the position at the endpoints:

s(3)=10(3)2+20=109+20=110 mms(3) = 10(3)^2 + 20 = 10 \cdot 9 + 20 = 110 \text{ mm}

s(0)=10(0)2+20=20 mms(0) = 10(0)^2 + 20 = 20 \text{ mm}

Thus, the displacement is:

Δs=s(3)s(0)=11020=90 mm\Delta s = s(3) - s(0) = 110 - 20 = 90 \text{ mm}

Distance Calculation

Since the velocity v(t)=20tv(t) = 20t is always positive over the interval [0,3][0, 3], the absolute value does not change the integral:

d=03v(t)dt=0320tdtd = \int_{0}^{3} |v(t)| \, dt = \int_{0}^{3} 20t \, dt

Evaluating this integral:

d=20[t22]03=20[920]=90 mmd = 20 \left[ \frac{t^2}{2} \right]_{0}^{3} = 20 \left[ \frac{9}{2} - 0 \right] = 90 \text{ mm}

In this case, both the displacement and the distance traveled are equal, as the particle does not change direction. However, if the velocity function had included negative values, the distance would have been greater than the displacement [average-velocity]. This illustrates why careful attention to the sign of velocity is essential when distinguishing between these two quantities in kinematic problems.

References

[velocity-function]

[position-function]

[acceleration-function]

[average-velocity]

AI Disclosure

This article was generated with the assistance of AI, which was used to structure and present the information derived from personal class notes. The content reflects the understanding of dynamics as taught in the course and is intended for educational purposes.

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