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Answers toStudent Questions

Physics

How to find total mechanical energy?

Mechanical energy is defined as the sum of an object’s energies due to its motion and position. The amount of mechanical energy an object possesses determines the amount of work it can do on other objects, or in other words, the amount of energy it is capable of transferring to other objects. Given the above definition, we can be more specific about the types of energy that contribute to the total mechanical energy of an object: - Kinetic energy $E_k$ is the energy associated with an object’s motion and is given by the formula $E_k = \dfrac{1}{2}mv^2$ where $m$ is the mass of the object and $v$ is its speed. Note that this is the macroscopic energy of motion of the particle, and does not include the microscopic energy of the movement of its particles which contributes to the object's internal energy. The energy associated with an object’s position is called its potential energy. Two main types of potential energy will contribute to mechanical energy: - Gravitational potential energy $E_p$ is the energy of an object due to its position in a gravitational field. For an object at a height $h$ above a reference point, its gravitational potential energy is calculated with the formula $E_p = mgh$, where $m$ is the mass of the object and $g$ is the gravitational field strength. At the Earth’s surface, the value for $g$ is 9.8 N kg$^{-1}$. - Elastic potential energy $E_H$ is is the energy stored due to the deformation of an elastic object. Work can be done in changing the shape of an object, for example stretching or compressing a string, and energy is stored in the object as a result. This stored energy is released when the object returns to its original shape. The standard formula for elastic potential energy is derived from Hooke's Law: $E_H = \dfrac{1}{2}kx^2$. Where $k$ is the spring constant and $x$ is the displacement from the equilibrium position. Another potential energy that can be considered to contribute to total mechanical energy is electric potential energy. Like gravitational potential energy, a charged object will have stored energy due to its position in an electric field. Because the idea of mechanical energy is normally applied to larger objects and not small charged particles, we will ignore it here. Having discussed the different types of energy that contribute to the mechanical energy of an object, we can create a formula for total mechanical energy. In words, the formula is $\hspace{3em} $ Mechanical Energy = Kinetic Energy + Potential Energy or more specifically $\hspace{3em} $ Mechanical Energy = Kinetic Energy + Gravitational Potential energy + Elastic Potential Energy In the form of an equation, the total mechanical energy can be expressed as $\hspace{3em} E_{tot}=E_k + E_p + E_H$ or $\hspace{3em} E_{tot}=\dfrac{1}{2}mv^2+ mgh+ \dfrac{1}{2}kx^2$

Economics

How does an increase in net exports shift the AD curve?

Aggregate demand (AD) is the total demand for an economy’s output at a given price level. It has four components: - Consumption (C): household spending on goods and services. - Investment (I): business spending on capital goods and raw materials. - Government spending (G): government purchases of goods and services (not transfers). - Net exports (NX): the value of exports (X) minus the value of imports (M). When any of these components increase, ceteris paribus, AD increases, shown by a rightward shift of the AD curve. For C, I, G, and exports, the relationship is straightforward: more spending on domestic output means higher AD. But it is less obvious why a fall in imports raises AD. Consider this example: If German households buy 5 German cars and 1 Japanese car, German output is 5 cars. Yet firms report sales as 6 cars, so consumption is recorded as the value of 6 cars. To avoid overstating domestic output, the value of the imported car is subtracted. In effect, imports are deducted from C, I, and G to ensure AD reflects demand for domestic production only. This is especially important with imported inputs. If a $\text{\textdollar}$100 belt is recorded as consumption but $\text{\textdollar}$20 of materials were imported, subtracting imports ensures AD reflects the $\text{\textdollar}$80 of domestic value added. Returning to the car example: if next year total car sales stay at 6 but imports fall to zero, consumption is unchanged, but domestic production must have risen from 5 to 6. In this case, households are substituting a domestically produced car for the previously imported one. Thus, lower imports—holding other components constant—mean greater demand for domestic output. In short: - If exports increase, foreign demand for domestic goods rises → AD increases. - If imports decrease (without a fall in C, I, or G), households or firms must be substituting toward domestic goods → AD increases. Therefore, when net exports increase—whether from higher exports or lower imports—aggregate demand increases, and the AD curve shifts to the right.

Mathematics

What is implicit differentiation?

Differentiation can be broadly divided into two categories: explicit differentiation and implicit differentiation. All the differentiation in the AI SL, AI HL and AA SL courses is explicit - we have a function entirely defined in terms of a single variable, and we can differentiate the function explicitly with respect to that variable. For example, the function $y=x^2 + 2x + 1$, or $f(x) = x^2 + 2x +1$, is a function of $x$, and can be differentiated explicitly with respect to $x$. $$ \begin{align*} \frac{\mathrm{d}y}{\mathrm{d}x} = 2x +2 \,\text{ or }\, f'(x) = 2x + 2 \end{align*} $$ In kinematics, the velocity function $v(t) = \sin (2t)$ is a function of $t$, and can be differentiated explicitly with respect to $t$. $$ \begin{align*} v'(t) &= 2\cos(2t) \end{align*} $$ In the AA HL course, you will encounter implicit differentiation. **This arises when we have an equation, or a relationship between two variables, that cannot be expressed as a function of a single variable**. For example, suppose we have the elliptical equation $x^2+y^2-xy=8$. This is not a function, it is a relation, and if we want to find the derivative with respect to $x$, we cannot do so explicitly, because the terms $y^2$ and $-xy$ are not functions of $x$. But we can treat them as functions of $x$ and differentiate them implicitly, using the chain rule (and the product rule). First consider the term $y^2$. We want to differentiate this with respect to $x$. That is, we want to find $\dfrac{\mathrm{d}}{\mathrm{d}x}\left(y^2\right)$. If we let $y = f(x)$, so that $\dfrac{\mathrm{d}y}{\mathrm{d}x} = f'(x)$, then what we are trying to find is $\dfrac{\mathrm{d}}{\mathrm{d}x}\left(f(x)\right)^2$. According to the chain rule, this would be $2f(x)f'(x)$. Substituting $y$ in place of $f(x)$ and $\dfrac{\mathrm{d}y}{\mathrm{d}x}$ in place of $f'(x)$ we have $$ \begin{align*} \dfrac{\mathrm{d}}{\mathrm{d}x}\left(y^2\right) &= 2f(x)f'(x)\\[8pt] &= 2y\dfrac{\mathrm{d}y}{\mathrm{d}x} \end{align*} $$ We have differentiated $y^2$ with respect to $x$ implicitly. Now consider the term $-xy$. Again let $y = f(x)$. We want to find $\dfrac{\mathrm{d}}{\mathrm{d}x}\left(-xy\right)$, which we can write as $\dfrac{\mathrm{d}}{\mathrm{d}x}\left(-xf(x)\right)$. Using the product rule, we have $\dfrac{\mathrm{d}}{\mathrm{d}x}\left(-xf(x)\right) = -f(x) -xf'(x)$. Substituting $y$ for $f(x)$ and $\dfrac{\mathrm{d}y}{\mathrm{d}x}$ for $f'(x)$ we have found our derivative implicitly. $$ \begin{align*} \frac{\mathrm{d}}{\mathrm{d}x}\left(-xy\right) &= -f(x) -xf'(x) \\[8pt] &= -y-x\frac{\mathrm{d}y}{\mathrm{d}x} \end{align*} $$ The other two terms, $x^2$ and $8$, can be differentiated explicitly. $$ \begin{align*} \frac{\mathrm{d}}{\mathrm{d}x}\left(x^2\right) &= 2x \\[8pt] \frac{\mathrm{d}}{\mathrm{d}x} (8) &= 0 \end{align*} $$ So once every term is differentiated we have $$ \begin{align*} 2x + 2y\frac{\mathrm{d}y}{\mathrm{d}x} -y-x\frac{\mathrm{d}y}{\mathrm{d}x} &= 0 \end{align*} $$ Finally, we can make $\dfrac{\mathrm{d}y}{\mathrm{d}x}$ the subject of the equation. $$ \begin{align*} \frac{\mathrm{d}y}{\mathrm{d}x} &= \frac{2x-y}{y-2x} \end{align*} $$ In general, if we have a function of $y$, but want to differentiate with respect to $x$, we can differentiate it with respect to $y$ then multiply by $\dfrac{\mathrm{d}y}{\mathrm{d}x}$, and that is a reasonable way to understand the implicit differentiation process in the AA HL course. $$ \begin{align*} \dfrac{\mathrm{d}}{\mathrm{d}x}f(y) &= f'(y)\,\dfrac{\mathrm{d}y}{\mathrm{d}x} \end{align*} $$

Biology

What is the role of acetylcholine in a skeletal muscle contraction?

Acetylcholine triggers skeletal muscle contraction by transmitting a nerve impulse across the neuromuscular junction, leading to muscle fiber depolarization. Understanding the role of acetylcholine (ACh) in skeletal muscle contraction is essential for grasping how nerve signals initiate and control movement. Acetylcholine is a neurotransmitter, a chemical messenger released by motor neurons at the neuromuscular junction—the synapse between a motor neuron and a skeletal muscle fiber. Its main function is to transmit the electrical signal from the neuron to the muscle, converting the neural signal into a muscle action. When an action potential (electrical impulse) reaches the end of a motor neuron, it causes voltage-gated calcium channels to open in the neuron’s membrane. Calcium ions enter the neuron, triggering synaptic vesicles filled with acetylcholine to fuse with the presynaptic membrane and release their contents into the synaptic cleft by exocytosis. This release is highly regulated and ensures that acetylcholine is only released in response to a signal. Once in the synaptic cleft, acetylcholine diffuses across the gap and binds to receptors on the sarcolemma (muscle cell membrane). These receptors are ligand-gated ion channels. Binding of acetylcholine opens the channels, allowing sodium ions (Naâș) to enter the muscle fiber and potassium ions (Kâș) to exit. This creates a local depolarization of the sarcolemma. If this depolarization reaches threshold, it triggers an action potential that spreads along the muscle fiber and into the T-tubules, initiating the process of muscle contraction. The muscle action potential ultimately leads to the release of calcium ions from the sarcoplasmic reticulum inside the muscle fiber. These calcium ions bind to troponin, shifting the tropomyosin and exposing the actin binding sites needed for cross-bridge formation with myosin—thus allowing the contraction cycle to proceed. Finally, acetylcholine must be quickly removed from the synaptic cleft to prevent continuous stimulation of the muscle. This is achieved by the enzyme acetylcholinesterase, which breaks down acetylcholine into acetate and choline. Choline is taken back up into the neuron to be recycled. This rapid breakdown ensures that each nerve signal leads to a single, controlled muscle contraction rather than prolonged or involuntary activity.

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