The electrical energy provided to a motor is determined by the power delivered to it, multiplied by the time for which the power is supplied. This can be expressed mathematically as:
\( E = V \times I \times t \)
Where:
Given the problem:
Substitute these values into the formula:
\( E = 12 \times 2.1 \times 1.5 \)
This gives:
\( E = 37.8 \, \text{J} \)
When rounded to two significant figures, the electrical energy transferred is approximately 38 J.
The gravitational potential energy (GPE) of an object at a certain height is given by the equation:
\( \text{GPE} = m \times g \times h \)
Where:
To find the gravitational potential energy gained by the mass, follow these steps:
\( 130 \, \text{g} = 0.130 \, \text{kg} \)
\( 63 \, \text{cm} = 0.63 \, \text{m} \)
\( \text{GPE} = 0.130 \, \text{kg} \times 9.81 \, \text{m/s}^2 \times 0.63 \, \text{m} \)
Multiplying these values:
\( \text{GPE} \approx 0.130 \times 9.81 \times 0.63 \approx 0.803 \, \text{J} \)
Rounded to two significant figures, the gravitational potential energy is approximately 0.80 J.
When analyzing the process of lifting a mass using a motor, it is essential to realize that the electrical energy provided to the system is not entirely converted into gravitational potential energy. Here are the key factors responsible for the discrepancy:
All these losses result in the gravitational potential energy (0.80 J) being less than the total electrical energy (38 J) delivered to the motor.
Parameter | Value | Unit | Calculation |
---|---|---|---|
Voltage (\(V\)) | 12 | V | Given |
Current (\(I\)) | 2.1 | A | Given |
Time (\(t\)) | 1.5 | s | Given |
Electrical Energy (\(E\)) | \(12 \times 2.1 \times 1.5 = 37.8\) → 38 | J | \( E = V \times I \times t \) |
Mass (\(m\)) | 0.130 | kg | \(130 \, \text{g} = 0.130 \, \text{kg}\) |
Height (\(h\)) | 0.63 | m | \(63 \, \text{cm} = 0.63 \, \text{m}\) |
Acceleration (\(g\)) | 9.81 | \(m/s^2\) | Standard value |
Gravitational Potential Energy (GPE) | \(0.130 \times 9.81 \times 0.63 \approx 0.80\) | J | \( \text{GPE} = m \times g \times h \) |
The problem presented serves as an example of how energy conversion is far from ideal in practical applications. While the electrical energy transferred to the motor is a straightforward product of voltage, current, and time, the work performed by the motor in lifting a mass illustrates a more complex interaction where only a fraction of the energy is utilized for the intended mechanical task.
This difference is a direct demonstration of the law of conservation of energy, where the energy that is not converted into useful mechanical energy is transformed into forms such as heat or acoustic energy. In engineering systems and physics experiments, understanding and quantifying these losses is critical in designing more efficient machines and in improving the theoretical models that predict system behavior.
Motors, whether they are used in industrial applications or simple educational experiments, seldom operate at 100% efficiency. Several factors contribute to the losses observed:
Engineers and designers must account for these losses when developing systems. By improving insulation, using higher quality materials, and designing better moving components, improvements in efficiency can be made. However, even in systems where efficiency is maximized, factors like friction and heat losses still ensure the output energy (in this case, the gravitational potential energy) remains lower than the input electrical energy.
Understanding these discrepancies is not only valuable from a theoretical standpoint but has practical implications as well. In applications ranging from industrial lift systems to electric vehicles, energy management and efficiency are critical design criteria. Improving these factors can lead to significant energy savings, reduced wear and tear on mechanical components, and extended system lifespans.
An example of practical importance can be seen in energy audits for machinery, where engineers measure both the energy input and the effective work output. Such analyses help in identifying areas where inefficiencies are most pronounced, guiding targeted improvements in equipment design and maintenance schedules.
This examination offers a comprehensive analysis of the motor-driven mass-lifting scenario. The electrical energy transferred to the motor is calculated using the formula \( E = V \times I \times t \) and is approximately 38 J when using the provided parameters. In parallel, the gravitational potential energy gained by a 130 g mass lifted by 63 cm is determined using \( \text{GPE} = m \times g \times h \), which comes out to nearly 0.80 J.
The substantial difference between these two energy values is attributed to inherent system inefficiencies. Losses due to friction, internal resistance, heat generation, and other processes ensure that only a fraction of the electrical energy contributes to increasing the gravitational potential energy of the mass. This scenario highlights fundamental principles in energy conservation and efficiency that are critical in both educational contexts and real-world engineering applications.
By analyzing and quantifying these factors, one gains essential insights into why practical systems stray from idealized models and what strategies can be adopted to enhance performance. It also underscores the importance of careful energy management in designing devices, as even small inefficiencies can have significant cumulative effects over time.