Problem 46
Question
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(x(t)=1+3 t, y(t)=2-6 t ; t_{1}=2\)
Step-by-Step Solution
Verified Answer
Both tangential and normal components of acceleration are 0 at \(t = 2\).
1Step 1: Find the velocity vector
To find the velocity vector, we differentiate the position vector components with respect to time \(t\). This gives us \(v(t) = \left(\frac{dx}{dt}, \frac{dy}{dt}\right)\). For \(x(t)=1+3t\) and \(y(t)=2-6t\), the derivatives are \(\frac{dx}{dt} = 3\) and \(\frac{dy}{dt} = -6\). Therefore, the velocity vector is \(v(t) = (3, -6)\).
2Step 2: Find the acceleration vector
The acceleration vector is found by differentiating the velocity vector components with respect to time \(t\). Since \(v(t) = (3, -6)\), both derivatives are zero, resulting in the acceleration vector \(a(t) = (0, 0)\).
3Step 3: Evaluate the velocity and acceleration at \(t_1 = 2\)
At \(t = t_1 = 2\), the velocity vector remains \(v(2) = (3, -6)\) and the acceleration vector remains \(a(2) = (0, 0)\) because they are both constant.
4Step 4: Calculate the magnitude of the velocity vector
The magnitude of the velocity vector is found using \(|v(t)| = \sqrt{(3)^2 + (-6)^2} = \sqrt{9 + 36} = \sqrt{45} = 3\sqrt{5}\).
5Step 5: Calculate the tangential component of acceleration
The tangential component of acceleration is given by \(a_T = \frac{d|v|}{dt}\). Since the velocity magnitude \(3\sqrt{5}\) is constant, its derivative is zero, so \(a_T = 0\).
6Step 6: Calculate the normal component of acceleration
The normal component of acceleration is given by \(a_N = \sqrt{|a(t)|^2 - a_T^2}\). Since \(a(t) = (0,0)\), we have \(|a(t)| = 0\) leading to \(a_N = \sqrt{0^2 - 0^2} = 0\).
Key Concepts
Velocity VectorAcceleration VectorDifferentiationMagnitude of Velocity
Velocity Vector
The velocity vector represents the rate of change of position in space over time. It's like capturing the direction and speed of an object as it moves. If you consider a path described by position functions such as \(x(t)\) and \(y(t)\), the velocity vector \(v(t)\) is found by differentiating these functions with respect to time \(t\).
For the given functions, \(x(t) = 1 + 3t\) and \(y(t) = 2 - 6t\), the differentiation yields \(\frac{dx}{dt} = 3\) and \(\frac{dy}{dt} = -6\).
Consequently, the velocity vector becomes \(v(t) = (3, -6)\).
The components of this vector, 3 and -6, tell us about the motion in the horizontal and vertical directions, respectively.
For the given functions, \(x(t) = 1 + 3t\) and \(y(t) = 2 - 6t\), the differentiation yields \(\frac{dx}{dt} = 3\) and \(\frac{dy}{dt} = -6\).
Consequently, the velocity vector becomes \(v(t) = (3, -6)\).
The components of this vector, 3 and -6, tell us about the motion in the horizontal and vertical directions, respectively.
- The horizontal velocity is constant at 3 units per time.
- The vertical velocity is constant at -6 units per time, indicating downward motion.
Acceleration Vector
The acceleration vector is a fundamental concept in understanding how velocity changes over time. This vector measures the rate of change of the velocity vector itself.
To find the acceleration vector, you differentiate the components of the velocity vector with respect to time \(t\).
Given that the velocity vector \(v(t) = (3, -6)\) holds constant values, the differentiation \(\frac{d}{dt} (3) = 0\) and \(\frac{d}{dt} (-6) = 0\) results in the acceleration vector \(a(t) = (0, 0)\).
Here are the highlights:
To find the acceleration vector, you differentiate the components of the velocity vector with respect to time \(t\).
Given that the velocity vector \(v(t) = (3, -6)\) holds constant values, the differentiation \(\frac{d}{dt} (3) = 0\) and \(\frac{d}{dt} (-6) = 0\) results in the acceleration vector \(a(t) = (0, 0)\).
Here are the highlights:
- The acceleration vector \((0,0)\) indicates no net change in velocity over time.
- In our case, this means steady-state motion without increase or decrease in speed in any direction.
Differentiation
Differentiation is a mathematical process you'll often use when working with vectors, such as velocity and acceleration.
In essence, it measures how a quantity changes over a small interval of time.
When you differentiate a function, you're essentially looking for its 'rate of change'. In the context of our exercise, you're applying differentiation one time to position functions to get velocity, and then again to those velocity functions to find acceleration.
Common steps include:
In essence, it measures how a quantity changes over a small interval of time.
When you differentiate a function, you're essentially looking for its 'rate of change'. In the context of our exercise, you're applying differentiation one time to position functions to get velocity, and then again to those velocity functions to find acceleration.
Common steps include:
- For position functions \(x(t)\) and \(y(t)\), differentiate with respect to \(t\) to find \(\frac{dx}{dt}\) and \(\frac{dy}{dt}\), forming the velocity vector \((v_x, v_y)\).
- Differentiate these velocity components with respect to time again to get the acceleration vector.
Magnitude of Velocity
The magnitude of a velocity vector essentially tells you the speed of the object. It is derived from the Pythagorean theorem and represents the overall speed without regard to direction.
For a velocity vector \(v(t) = (v_x, v_y)\), the magnitude is calculated as:
\[ |v(t)| = \sqrt{v_x^2 + v_y^2} \]
In our example, with \(v(t) = (3, -6)\), the magnitude is \(\sqrt{(3)^2 + (-6)^2} = \sqrt{9 + 36} = \sqrt{45} = 3\sqrt{5}\).
Key points about the magnitude of velocity:
For a velocity vector \(v(t) = (v_x, v_y)\), the magnitude is calculated as:
\[ |v(t)| = \sqrt{v_x^2 + v_y^2} \]
In our example, with \(v(t) = (3, -6)\), the magnitude is \(\sqrt{(3)^2 + (-6)^2} = \sqrt{9 + 36} = \sqrt{45} = 3\sqrt{5}\).
Key points about the magnitude of velocity:
- It provides a scalar value, the speed, representing how fast an object is moving.
- A constant magnitude, like in our example, indicates steady speed over time.
Other exercises in this chapter
Problem 45
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}
View solution Problem 45
The solid spheres \((x-1)^{2}+(y-2)^{2}+(z-1)^{2} \leq 4\) and \((x-2)^{2}+(y-4)^{2}+(z-3)^{2} \leq 4\) intersect in a solid. Find its volume.
View solution Problem 47
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left
View solution Problem 47
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}
View solution