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Answers toStudent Questions

Biology

What does starch do for a plant?

Starch plays a vital role in plants by serving as a storage form of glucose. During photosynthesis, plants often produce more glucose than they immediately require. To manage this surplus, they convert the excess glucose into starch—a carbohydrate that can be hydrolysed and respired to release energy when needed. This stored energy supports essential processes such as growth, repair, and survival, particularly when photosynthesis slows or stops, such as at night or during winter. Biochemically, starch is composed of two types of polysaccharides: amylose and amylopectin. Amylose consists of alpha-glucose units joined by α 1-4 glycosidic bonds, forming a linear, coiled structure. Amylopectin, by contrast, is branched and contains both α 1-4 and α 1-6 glycosidic linkages between the alpha-glucose molecules. The α-1,6 glycosidic linkages cause branching, which allows amylopectin to be broken down more rapidly than amylose. This structural difference makes amylopectin particularly useful when the plant needs to quickly access stored glucose. Starch is typically stored in organs such as roots, seeds, tubers, and some leaves. When environmental conditions limit photosynthesis, the plant hydrolyses starch back into glucose. This glucose is then used in cellular respiration to generate ATP, providing energy for vital metabolic activities. Because starch is insoluble, it does not affect the osmotic potential of the cell where it is stored, allowing glucose to be stored without disrupting water balance. This property allows plants to store large quantities of glucose without disrupting cellular function or water potential. In summary, starch enables plants to maintain a stable and accessible energy reserve. Its biochemical structure, efficient storage capacity, and osmotic neutrality make it ideal for managing energy needs when photosynthetic activity is reduced. This function is fundamental to plant survival, development, and adaptation to changing environmental conditions.

Physics

Why does v = fλ?

The universal wave equation v = fλ is one of the fundamental equations in Physics. It relates the speed of a wave, v, the frequency, f, and the wavelength λ. Waves are periodic disturbances that propagate energy through a medium. They are caused by an oscillating source that creates the original disturbance. The frequency of the resulting wave is equal to the frequency of the source. The period $T$ of the oscillation is the inverse of the frequency $f$. One period is the time that it takes for the source to complete a full cycle and return to its original position. The particles in the medium propagate the wave through individual oscillations with this same period. The wavelength $\lambda$ of a wave is defined as the distance between two successive points on a wave that are oscillating in phase. An example of points on a transverse wave that are in phase with each other are crests - at a crest the particles are at the top of their oscillatory motion. Similarly, all points on troughs are in phase with each other. So the distance between adjacent crests or troughs is one wavelength. For a longitudinal wave, a wavelength is the distance between the centers of two adjacent compressions or rarefactions. Now we can think about how far a wave travels in the time that it takes the source disturbance to repeat itself, or in other words, complete one cycle. The time for one cycle is the period $T$. Waves will travel away from the source at a speed $v$. This speed depends on the nature of the medium and is independent of the frequency of the source. If we consider a wave that travels away from the oscillating source, we can use the speed equation $v = \dfrac{s}{t}$ to determine that the distance $s$ that the wave travels in one period $T$ is given by $\hspace{3em} s = vT $ This distance is the separation between two repeating points on the waveform, and so is equal to the wavelength $\lambda$ $\hspace{3em} λ = vT$ Solving for the speed gives $\hspace{3em} v = \dfrac{\lambda}{T}$ And we know that the period is the inverse of the frequency $\hspace{3em}T = \dfrac{1}{f}$ Substituting in, we arrive at the wave equation $\hspace{3em} v = f \lambda$

Biology

Which law explains how alleles separate during gamete formation?

When studying the inheritance of a single gene, Mendel's Law of Segregation explains how the alleles for that gene separate during gamete formation.. This law states that alleles for different genes assort independently during gamete formation, provided the genes are located on different chromosomes. Each individual has two alleles for a gene, one inherited from the biological mother and one from the biological father. These alleles are separated during meiosis, which is the process of nuclear division that produces haploid gametes. $\underline{\textrm{Meiosis I: Separation of alleles}}$: Before meiosis begins, each chromosome makes an identical copy of itself, known as **sister chromatids**, which are joined together at the **centromere**. During **prophase I**, the chromosomes condense and become visible, forming **tetrads** (pairs of homologous chromosomes), each consisting of two sister chromatids. These homologous chromosomes line up, in their tetrads, across the equator of the cell during **metaphase I**. In **anaphase I**, the homologous chromosomes are pulled to opposite poles of the cell. Importantly, the sister chromatids remain attached during this phase. This ensures that each resulting cell will contain only one allele from each gene pair. The separation of homologous chromosomes during **meiosis I** explains **Mendel's Law of Segregation**, which states that alleles for a gene separate during gamete formation. For example, if an individual has the genotype **Aa** for a gene, the **A** and **a** alleles will be carried on different homologous chromosomes. During meiosis I, these chromosomes are separated, so the resulting two cells will contain either **A** or **a**, but not both. The **Law of Independent Assortment** also occurs during meiosis I, specifically during metaphase I, when homologous chromosomes align randomly along the equator of the cell. During anaphase I, these chromosomes are separated to opposite poles of the cell. However, this law does not explain the separation of alleles for a single gene; rather, it explains the **genetic variation** that results from the independent assortment of alleles for different genes located on different chromosomes. $\underline{\textrm{Meiosis II: Formation of Gametes and Separating Sister Chromatids}}$: After **meiosis I**, the two haploid cells enter **meiosis II**. During **metaphase II** the pairs of sister chromatids form a single line across the equator of the cell. In **anaphase II**, the centromeres split, and the sister chromatids (now regarded as individual chromosomes) are pulled to opposite poles of the cell. This ensures that each **gamete** will contain a single **chromosome** from each pair, contributing to the haploid number of chromosomes. The result of meiosis II is the formation of **four non-identical haploid gametes**, each containing one allele for each gene. In summary, **Mendel's Law of Segregation** explains the separation of homologous chromosomes during meiosis I, which ensures that each gamete carries only one allele for each gene. **Mendel's Law of Independent Assortment** explains how genetic variation is increased by the independent inheritance of alleles for different genes, depending on their location on different chromosomes.

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