Motion in One Dimension
1.0 Introduction
2.0 Kinematic variables
2.1 Distance and displacement
2.2 Average speed and velocity
2.3 Instantaneous speed and velocity
2.4 Average and instantaneous acceleration
3.0 Motion in one dimension
3.1 Motion in a straight line with uniform velocity
3.2 Motion in a straight line with uniform acceleration
3.3 Motion in a straight line with non-uniform acceleration
4.0 Derivation of the kinematics equation
5.0 Vertical motion under gravity
5.1 Basic terminologies for motion under gravity
5.2 Detailed concept of motion under gravity
5.3 Solved examples
6.0 Analysis of motion through graph
6.1 Displacement - time graph
6.2 Velocity - time graph
6.3 Area under the graph
6.4 Solved examples
7.0 Relative motion
7.1 Relative displacement
7.2 Relative velocity
7.3 Relative acceleration
7.4 Illustration of relative motion
7.5 Application of relative motion
8.0 Simultaneous motion of two bodies
9.0 River boat problem
9.1 Downstream
9.2 Upstream
9.3 Crosses the river in shortest interval of time
9.4 Reaches the point just opposite from where he started
9.5 River-man problem
9.6 Solved examples
10.0 Aircraft-wind problem
11.0 Rain problem
6.1 Displacement - time graph
2.2 Average speed and velocity
2.3 Instantaneous speed and velocity
2.4 Average and instantaneous acceleration
3.2 Motion in a straight line with uniform acceleration
3.3 Motion in a straight line with non-uniform acceleration
5.2 Detailed concept of motion under gravity
5.3 Solved examples
6.2 Velocity - time graph
6.3 Area under the graph
6.4 Solved examples
7.2 Relative velocity
7.3 Relative acceleration
7.4 Illustration of relative motion
7.5 Application of relative motion
9.2 Upstream
9.3 Crosses the river in shortest interval of time
9.4 Reaches the point just opposite from where he started
9.5 River-man problem
9.6 Solved examples
As we know, $$\frac{{ds}}{{dt}} = v$$ and $$\frac{{{d^2}s}}{{d{t^2}}} = a$$
S. No. | Type of motion | Graph | Explanation |
1. | Body is stationary | Slope is $0$, $$\frac{{ds}}{{dt}} = 0$$ So, $v=0$ Also, it is a straight line. $$\frac{{{d^2}s}}{{d{t^2}}} = 0$$ So, $$a = 0$$ | |
2. | Uniform motion | As slope is constant. So, $$v = \frac{{ds}}{{dt}}$$$$v = {\text{constant}}$$ Also, it is a straight line. So, $$\frac{{{d^2}s}}{{d{t^2}}} = 0$$$$a = 0$$ | |
3. | Uniformly acceleration motion | As we can see that slope changes at every point in a curve. So, velocity is variable. $$v = \frac{{ds}}{{dt}} = {\text{variable}}$$ As the curve is concave up. So, the acceleration is positive. $$a = \frac{{{d^2}s}}{{d{t^2}}} > 0$$ If acceleration is positive, velocity will increase. | |
4. | Uniformly retarded motion | As we can see that slope changes at every point in a curve. So, velocity is variable. $$v = \frac{{ds}}{{dt}} = {\text{variable}}$$ As the curve is concave down. So, the acceleration is negative. $$a = \frac{{{d^2}s}}{{d{t^2}}} < 0$$ If acceleration is negative, velocity will decrease. | |
5. | Uniform motion | e$$v = \frac{{ds}}{{dt}} = {\text{constant}}$$$$\tan \theta = - ve$$ So, velocity is in negative direction or we can say it is moving towards the observer. Acceleration is $0$, as the curve is a straight line. $$\frac{{{d^2}s}}{{d{t^2}}} = 0$$ So, $$a = 0$$ |