Problem 33
Question
A small block with mass 0.0400 kg is moving in the \(xy\)-plane. The net force on the block is described by the potentialenergy function \(U(x, y) = (5.80 \, \mathrm{J/m}^2)x^2 - (3.60 \, \mathrm{J/m}^3)y^3\). What are the magnitude and direction of the acceleration of the block when it is at the point (\(x =\) 0.300 m, \(y =\) 0.600 m)?
Step-by-Step Solution
Verified Answer
The magnitude is \( 5.72 \ \mathrm{m/s}^2\) and the direction is \( 92.5^\circ \) from the x-axis.
1Step 1: Identify given quantities
Extract initial velocity, acceleration, time, displacement.
2Step 2: Choose kinematic equation
Use v=v0+at, x=v0t+0.5at^2, or v^2=v0^2+2a*dx.
3Step 3: Substitute and solve
Plug in values and solve.
4Step 4: State the answer
The answer is: The magnitude is \( 5.72 \ \mathrm{m/s}^2\) and the direction is \( 92.5^\circ \) from the x-axis.
Key Concepts
Potential EnergyForce ComponentsAcceleration CalculationGradient of a Function
Potential Energy
Potential energy is a concept in physics that refers to the energy stored in an object due to its position or configuration. In classical mechanics, potential energy is often associated with objects under the influence of gravitational, elastic, or electrical forces.
In the example given, the potential energy function, which depends on the "x" and "y" coordinates, signifies the energy stemming from a combination of forces acting on the block. Potential energy functions allow the calculation of force exerted on an object by applying derivatives (more on this shortly). The potential energy function used in this problem contains terms for both the "x" and "y" directions:
In the example given, the potential energy function, which depends on the "x" and "y" coordinates, signifies the energy stemming from a combination of forces acting on the block. Potential energy functions allow the calculation of force exerted on an object by applying derivatives (more on this shortly). The potential energy function used in this problem contains terms for both the "x" and "y" directions:
- For the "x" direction: \((5.80 \, \mathrm{J/m}^2)x^2\)
- For the "y" direction: \(-(3.60 \, \mathrm{J/m}^3)y^3\).
Force Components
Understanding force components is crucial for analyzing motion in more than one dimension, like in the given problem. Forces can be resolved into components to simplify calculations and understand how they act. In this scenario, forces in the "x" and "y" directions can be derived from the potential energy function using its gradient.
The gradient is a vector that indicates the direction and rate of the fastest increase of a function. To find the force components related to a potential energy function, we use negative partial derivatives. The equations are:
The gradient is a vector that indicates the direction and rate of the fastest increase of a function. To find the force components related to a potential energy function, we use negative partial derivatives. The equations are:
- For the "x" component of force \(F_x\): \(F_x = -\frac{\partial U}{\partial x}\) = \( -2(5.80 \, \mathrm{J/m}^2)x = -11.6x \, \mathrm{J/m}^2 \)
- For the "y" component of force \(F_y\): \( F_y = -\frac{\partial U}{\partial y}\) = \( 3(3.60 \, \mathrm{J/m}^3)y^2 = 10.8y^2 \, \mathrm{J/m}^2 \)
Acceleration Calculation
Once the force components are determined, calculating acceleration becomes a straightforward task in classical mechanics. According to Newton's second law of motion, the net force acting on an object is equal to the mass of the object times its acceleration. This can be expressed as:
\[ F = ma \]
Where "F" is the total force, "m" is the mass, and "a" is the acceleration. If we have components for force, acceleration can be likewise decomposed into components:
\[ F = ma \]
Where "F" is the total force, "m" is the mass, and "a" is the acceleration. If we have components for force, acceleration can be likewise decomposed into components:
- \( a_x = \frac{F_x}{m} \)
- \( a_y = \frac{F_y}{m} \)
Gradient of a Function
The gradient of a function is a powerful mathematical tool for understanding how a function changes. In more basic terms, it is a vector composed of the function’s partial derivatives with respect to each variable. It points in the direction of fastest increase of the function and its magnitude represents the rate of increase.
When applied to a potential energy function, the gradient helps identify force directions. This is crucial because in mechanics, force and potential energy are closely related by the negative gradient:
When applied to a potential energy function, the gradient helps identify force directions. This is crucial because in mechanics, force and potential energy are closely related by the negative gradient:
- \( abla U(x,y) = \left( \frac{\partial U}{\partial x}, \frac{\partial U}{\partial y} \right) \)
Other exercises in this chapter
Problem 31
A force parallel to the \(x\)-axis acts on a particle moving along the x-axis. This force produces potential energy \(U(x)\) given by \(U(x) = \alpha x^4\), whe
View solution Problem 32
The potential energy of a pair of hydrogen atoms separated by a large distance \(x\) is given by \(U(x) = -C_6/x^6\), where \(C_6\) is a positive constant. What
View solution Problem 34
An object moving in the \(xy\)-plane is acted on by a conservative force described by the potential-energy function \(U(x, y) = \alpha[(1/x^2) + (1/y^2)]\), whe
View solution Problem 35
The potential energy of two atoms in a diatomic molecule is approximated by \(U(r) = (a/r^{12}) - (b/r^6)\), where \(r\) is the spacing between atoms and \(a\)
View solution